FINAL DRAFT JULY 2017

1

NOT TO BE REFERENCED

Report No. XX

2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42

OPERATIONAL QUANTITIES FOR
EXTERNAL RADIATION EXPOSURE

Joint report of

THE INTERNATIONAL COMMISSION ON
RADIATION UNITS AND
MEASUREMENTS
andTHE INTERNATIONAL COMMISSION ON
RADIOLOGICAL PROTECTIONMONTH 2017

Journal of the ICRU Volume XX No X 2017
ISBN XXXXXXXXXX
Published by Oxford University Press

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

43
44
45
46
47

OPERATIONAL QUANTITIES FOR
EXTERNAL RADIATION EXPOSURE

48
49
50
51
52
53
54
55
56
57
58
59

Report Committee

60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84

N.E.Hertel (Co-Chair), Georgia Institute of Technology, USA.
D.T. Bartlett (Co-Chair), Abingdon, UK
R.Behrens, Physikalisch-Technische Bundesanstalt, Braunschweig, Germany
J-M.Bordy, CEA, LIST, Laboratoire National Henri Becquerel (LNE-LNHB), 91191 Gif-sur-Yvette,
France†G..Dietze , Braunschweig, Germany
A. Endo, Japan Atomic Energy Agency, Japan
G.Gualdrini, Ente per le Nuove Tecnologie, L’Energia e L’Ambiente, Bologna, Italy (until 2015)
T. Otto, European Organization for Nuclear Research (CERN), Geneva, Switzerland
M.Pelliccioni, Istituto Nazionale di Fisica Nucleare, Frascati, Italy

Consultants to the Report Committee
P. Ambrosi, Physikalisch-Technische Bundesanstalt, Braunschweig, Germany (until 2014)
M.B.Bellamy, Center for Radiation Protection Knowledge, Oak Ridge National Laboratory, Oak
Ridge, USA
J-F. Bottollier-Depois, Institut de Radioprotection et de Sûreté Nucléaire,
Fontenay-aux-Roses, France
J. Daures, CEA, LIST, Laboratoire National Henri Becquerel (LNE-LNHB), 91191 Gif-sur-Yvette,
FranceK.F.Eckerman, Oak Ridge, USA
P. Ferrari, Ente per le Nuove Tecnologie, L’Energia e L’Ambiente, Bologna, Italy
B.R.L. Siebert, Braunschweig, Germany
K.G. Veinot, Y-12 National Security Complex, Oak Ridge, USA

ICRU Sponsors
D.T. Burns, Bureau International des Poids et Mesures, Sèvres, France
E. Fantuzzi, Ente per le Nuove Tecnologie, L’Energia e L’Ambiente, Bologna, Italy
H-G. Menzel, Heidelberg, Germany†

Deceased. Dr Dietze played an important role in thedevelepment of the recommendations of thisReport. The Commission wishes to acknowledge
the loss resulting from his untimely death on 25th
January 2015 .

FINAL DRAFT JULY 2017

85
86

NOT TO BE REFERENCED

Dedication to Günther Dietze

87
88
89

Dr. Günther Dietze died on the 25th of January, 2015.

90

Günther was a member of the International Commission on Radiation Units and Measurements

91(ICRU) Fundamental Quantities and Units Committee, which recently published Report 85a

92

Fundamental Quantities and Units for Ionizing Radiation, and was on the ICRU Committees that93

prepared Report 47 Measurement of Dose from External Photon and Electron Radiations, and94

Report 57 Conversion Coefficients for use in Radiological Protection Against External Radiation. He

95

contributed strongly to the preparation of this Report.

96

At the Physikalisch-Technische Bundesanstalt (PTB), Braunschweig, he was Head of the

97

Ionizing Radiation Division, with responsibility for radioactivity, dose measurements for medical

98

applications, radiation protection dosimetry, and neutron metrology. He had a strong interest in99

neutron dosimetry, publishing many papers on detectors and spectrometers. He was a member of, and100

later led the German Radiation Protection Commission, and was a member of the Group of Experts

101

established under Article 31 of the EURATOM treaty. He was one of the first Council Members of

102

EURADOS, and was Chairman from 1991 to 2001.

103

Günther served on many national and international committees, and was a member of the

104

International Commission on Radiological Protection Committee 2, contributing significantly to Task

105

Groups, and to the Committees that prepared several publications including Publication 103, The

106

2007 Recommendations of the International Commission on Radiological Protection, and was

107

Chairman of the Committee that prepared Publication 123, Assessment of Radiation Exposure of108

Astronauts in Space. He was a Consultant Editor of the journal Radiation Protection Dosimetry.

109

Günther’s death is a significant loss to the dosimetry community.

FINAL DRAFT JULY 2017110

Operational Quantities for External Radiation Exposure

111
112

Preface

113

Abstract

114

Executive Summary

115

1

Introduction

116

2Concepts and Terms

NOT TO BE REFERENCED

117

2.1 Particle Energy

118

2.2 Charged Particle Equilibrium

119

2.3 ICRU 4-Element (soft) Tissue120

2.4 ICRU Sphere121

2.5 ICRP and ICRU Adult Anthropomorphic Reference Computational Phantoms

122

2.6 Conversion Coefficients

123
124

3

Definitions of Quantities
3.1 Radiometric Quantities

125

3.1.1

Fluence

126

3.1.2

Fluence Rate

127

3.1.3

Particle Radiance

128

3.2 Dosimetric Quantities

129

3.2.1

Kerma

130

3.2.2

Absorbed Dose131

3.3 Protection Quantities

132

3.3.1 Mean Absorbed Dose in an Organ or Tissue

133

3.3.2 Effective Dose134

3.4 Operational Quantities for External Exposure

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

135

3.4.1 Ambient Dose

136

3.4.2 Ambient Dose Rate

137

3.4.3 Directional Absorbed Dose in the Lens of the Eye

138

3.4.4 Directional Absorbed Dose in the Lens of the Eye Rate

139

3.4.5 Directional Absorbed Dose in Local Skin

140

3.4.6 Directional Absorbed Dose in Local Skin Rate

141

3.4.7 Personal Dose

142

3.4.8 Personal Absorbed Dose in the Lens of the Eye

143

3.4.9 Personal Absorbed Dose in Local Skin

144

4

Conversion Coefficients145

4.1Conversion Coefficients for the Operational Quantities

146

4.2 Comparison of Quantities of Values Recommended and Previous Conversion

147

Coefficients

148

4.2.1General Remarks

149

4.2.2 Ambient and Personal Dose

150

4.2.3 Directional and Personal Absorbed Dose in the Lens of the Eye

151

4.2.4 Directional and Personal Absorbed Dose in Local Skin

152

5 Applications of Operational Quantities

153

5.1 Operational Quantities and their Application in Occupational Radiation Protection

154

5.2 Operational Quantities and their Application in Environmental Monitoring155

6 Calibration of Area Monitoring Instruments and Personal Dosimeters

156

6.1 General

157

6.2 Calibration Phantoms for Personal Dosimeters

158

FINAL DRAFT JULY 2017159

7 Conclusions

160

Appendix A Values of Conversion CoefficientsNOT TO BE REFERENCED

161

A.1 Ambient Dose162

A.2 Personal Dose163

A.3 Directional and Personal Absorbed Dose in the Lens of the Eye

164

A.4 Directional and Personal Absorbed Dose in Local Skin

165

A.5 Operational Quantities for Photons for Energies up to 50MeV Calculated with the166

Kerma-Approximation Method

167

A.6 Air Kerma

168

Appendix B Descriptions of Codes

169

B.1 PHITS

170

B.2 FLUKA

171

B.3 MCNP

172

B.4 EGSnrc

173

B.5 Revised Stopping Powers

174

Appendix C Informative: Alternative Conversion Coefficients for the Absorbed Dose in the Lens

175of the Eye

176

C.1 Directional and Personal Absorbed Dose in the Lens of the Eye, Maximum of Sensitive cells or

177

Complete Lens

178

C.2 Photons for Energies up to 50MeV Calculated with the Kerma-Approximation Method

179

References

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

Preface180
181

The International Commission on Radiological Protection, (ICRP), recommends protection

182

quantities for dose limits of occupationally exposed persons and members of the public, and for the183

optimization of radiation protection (ICRP, 2007). The quantities are not point quantities, and are not184

appropriate for the calibration of instruments for area and individual dose measurements. A second

185class of quantities, operational dose quantities, has been defined by ICRU for this purpose. These are186

point quantities. In principle, determinations by instruments of the operational quantities, to which

187

quantities instruments are calibrated and type tested, will provide estimates of the protection

188

quantities for particular radiation exposures.

189

Absorbed dose index and dose equivalent index were recommended in ICRU Report 19 (ICRU,

1901971) as the operational quantities for exposure to external radiation. In ICRU Report 20 (ICRU,

1911971) there is consideration of the use of MADE (maximum dose equivalent in an irradiated body).

192

Further development of the operational quantities was made in Report 39 (ICRU, 1985) and Report193

43 (ICRU, 1988). These Reports defined ambient dose equivalent, directional dose equivalent, and194

individual dose equivalent, as operational quantities that were then partly modified in ICRU Report

195

51 (ICRU, 1993). Information on the application of these quantities was given for photons and196

electrons in ICRU Report 47 (ICRU, 1992) and for neutrons in Report 66 (ICRU, 2001). Sets of

197

values of conversion coefficients from radiometric and dosimetric quantities were given in ICRU

198

Report 57 (ICRU, 1998), published jointly with ICRP in Publication 74 (ICRP, 1996).

199

The operational quantities previously recommended were based on dose equivalent at a point in200

the ICRU sphere and on dose equivalent at a point in the body. The quantities recommended in this201

Report are defined as radiometric and dosimetric quantities at a point multiplied by conversion

202

coefficients; the conversion coefficients are based on values of the protection quantities effective203

dose, absorbed dose in the lens of the eye, and absorbed dose in local skin.

204

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

Abstract

205
206

The Commission defines a set of operational dose quantities for the determination of the207

exposure of external radiation by measurement or calculation. These assessments serve as estimates

208

of values of the protection quantities defined by the International Commission on Radiological209

Protection (ICRP) that are generally not measurable. The set of ICRU operational dose quantities in

210

current use was defined 30 years ago.

211

The rationale for operational quantities has been examined taking into account the recent

212changes in the definitions of the protection quantities (ICRP, 2010); the changes in the fields of213

application of the operational quantities and protection quantities in medicine, scientific research, and214

natural sources of radiation; and the extension of types of particles and range of energies contributing

215

to doses to workers and members of the public. The previous operational quantities were based on the216

dose equivalent that would be produced at a depth in the hypothetical ICRU 4-element sphere, and on

217

dose equivalent in soft tissue at a point in the body. The investigations which have been carried out

218

that have led to the recommendations given in this Report have included the study the values of219

weighted absorbed doses at different depths in tissue-equivalent phantoms and the combination of

220

different depths. The operational quantities recommended in this Report are defined in terms of221radiometric and dosimetric quantities at a point in space multiplied by values of conversion

222

coefficients to the protection quantities, effective dose, absorbed dose in the lens of the eye, and223

absorbed dose in local skin, calculated for broad parallel beams incident on the body. The

224

relationship of the recommended operational quantities to the protection quantities has been225

investigated. The impact of changes on routine measurement practice, including instrument design226

and calibration has been considered.

227

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

228

Executive Summary

229

This Report considers in Section 1 the background of the use of protection quantities and230

operational quantities for the quantification of the exposure of the human body to ionizing radiation.

231

The protection quantities have been revised, owing partly to the changes in application and partly to the232

changes in the particle types and range of energies involved. The operational quantities require revision

233

for these reasons, but also for the limitations of the previous quantities. The concepts and terms used in234

this Report are explained in Section 2, and the definitions of the relevant radiometric and dosimetric235

quantities, the protection and the operational quantities for radiation protection of external exposure are236

given in Section 3. The recommended operational quantities for area monitoring are ambient dose,237

directional absorbed dose to the lens of the eye and directional absorbed dose to local skin; for238

individual monitoring personal dose, personal absorbed dose to the lens of the eye and personal239

absorbed dose to local skin. In Section 4, information is given on the method of computation of the240

recommended quantities is given. Comparisons are made between the recommended and previous

241

values of the conversion coefficients. These comparisons show the limitations of the previous quantities.

242

Section 5 considers the areas of application of the operational quantities in occupational radiation

243

protection and in environmental monitoring. The calibration of area monitoring instruments and244

personal dosimeters are considered in Section 6 with information on calibration procedures and the245calibration phantoms.

246

recommended operational quantities that overcome the limitations of the previous quantities and provide

247

a solution to the protection problems in radiation fields of higher-energy photons, electrons and neutrons,

248

and for other particle types.

Section 7 gives the general conclusions on the improvements of the

249

Appendix A gives values of the conversion coefficients to ambient dose, personal dose,250

directional absorbed dose in the lens of the eye, directional absorbed dose in local skin, personal

251

absorbed dose in the lens of the eye, and personal absorbed dose in local skin from particle fluence.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

252

For photons, two additional data sets of conversion coefficients are given: to the operational

253

quantities from air kerma; and to the operational quantities from fluence or air kerma calculated using254

the kerma-approximation method to approach charged-particle equilibrium. In Appendix B there are255

brief descriptions of the computer codes used for the calculation of these values. Informative tables

256

and figures are given in Appendix C to the maximum value of the absorbed dose in the lens of the257

eye to the sensitive cells or the complete lens from particle fluence, and for photons from air kerma.

258

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

259

1 Introduction

260

Radiological protection requires the quantification of the extent of exposure of the human body261

to ionizing radiation. To this end, the International Commission on Radiological Protection (ICRP)

262

developed the protection quantities, mean absorbed dose in an organ or tissue, equivalent dose in an

263

organ or tissue, and effective dose (ICRP, 1977, 1991, 2007). The protection quantities are used for264

the implementation of dose limits and for guiding quantitatively the optimization principles. The

265

latest data set of conversion coefficients from particle fluence to the protection quantities was

266

recommended in ICRP Publication 116 (ICRP, 2010), which was jointly published with the267

International Commission on Radiation Units and Measurements (ICRU). The conversion

268

coefficients of ICRP Publication 116 are calculated based on the definition of the protection

269

quantities in the 2007 Recommendations of the ICRP (ICRP, 2007). ICRP Publication 116 extends

270

radiation type and energy range of conversion coefficients in comparison with ICRP Publication 74

271(ICRP, 1996) and ICRU Report 57 (ICRU, 1998) and supersedes the conversion coefficients for the272

protection quantities in these Reports. Human-body-related protection quantities are defined in

273

organs and tissues and are not measurable in practice; therefore, they cannot be used directly as

274

quantities in radiation monitoring. The ICRU has developed a set of operational quantities to be used

275

in radiation measurements for external exposure to estimate the protection quantities. The current

276

operational quantities in use were defined in the 1980s (ICRU, 1985, 1988) and have been applied in

277

many countries under radiological protection directives and regulations over the past 30 years. The

278

previous system of operational quantities has some limitations (Bartlett and Dietze, 2010; Bartlett et279al., 2013) and needs further improvements to consider changes in the fields of application, including280

the extension of radiation type and energy range (ICRP, 2007, 2010, 2016; ICRU, 2010). The

281

determination of an operational quantity should give a value that is a close estimate of the value of282

the protection quantity.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

283

This Report recommends a redefinition of the operational quantities as the products of284

radiometric or dosimetric quantities at a point in space or on the surface of the body and conversion

285

coefficients related to values of protection quantities (Endo, 2016a). Consideration on this approach286

has been given previously (see, for example, Sidwell et al., 1969; ICRP Publication 15 (ICRP, 1969);

287

NCRP Report 38 (NCRP,1971); Burlin and Wheatley, 1971; Commission of the European

288

Communities (CEC, 1983); ICRP Publication 21 (ICRP, 1973); Burlin, Davies, and Wheatley, 1979;

289

Burlin, 1981; Jahr et al., 1981; Siebert and Bartlett, 1995). The practical application of such a

290

quantity can be made if conversion coefficients to an internationally agreed phantom exist. ICRP and

291

ICRU have now defined ICRP/ICRU adult reference phantoms in ICRP Publication 110 (ICRP,

2922009) that are widely accepted. These phantoms are used to define reference values of conversion

293

coefficients to the protection quantities and can be used to define the operational quantities. The

294

recommended operational quantities simplify the systems of protection and operational quantities,

295

and assists in the comprehension of radiological protection quantities by users.

296
297
298

Figure1: Scheme of relationships of quantities

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

299

The ICRP protection quantity effective dose is considered to provide a single risk-related

300

quantity for stochastic radiation effects, valid for all adult persons exposed under the same

301

conditions, independent of sex, age, size, and other individual properties of the person exposed.

302

Internal exposure from the intake of radionuclides can also be considered using this effective-dose

303

concept. The quantity effective dose is for consideration of stochastic effects at doses below 100 mSv

304

for setting exposure limits and for optimization. At higher values of dose, tissue reactions

305(deterministic effects) are of concern, and absorbed doses are to be evaluated (Harrison et al, 2016).

306

For evaluating tissue reactions, mean absorbed dose in the organ or tissue is assessed, weighted for307

high-LET radiation by a specific RBE. The RBE values will depend on the radiation type and energy,308

and can differ for different biological endpoints and different organs or tissues (ICRP, 2007).

309

For doses below dose constraints or investigation levels, in common practice, the protection

310

quantities are assessed in terms of the operational quantities. There is the possibility of significant

311

sources of uncertainty in the assessment of the protection quantities from the operational quantities

312[“Determination of protection quantities based on different knowledge of external exposure” German

313

booklet need reference]. To assess a more precise value and its uncertainty as doses approach the314constraints or investigation levels, information will be needed on the types of radiation involved, the315

uniformity of the radiation field and of its energy and direction distributions, the position of the316

instrument or dosimeter and its response characteristics, and whether the exposure is partial or whole-317

body. In some instances, additional information can be obtained by computer simulation of the318

exposure situation.

319

This Report provides a set of conversion coefficients from fluence to the operational quantities

320

for the particles photons, neutrons, electrons, positrons, protons, negative and positive muons,321

negative and positive pions, and helium ions, for energies up to 200 GeV, and also from air kerma for322

photons to 50 MeV. Conversion coefficients to the protection quantities for a few field geometries are

323

provided in ICRP Publication 116 (ICRP, 2010). However, more data for additional incident angles of

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

324

incidence that are not provided by ICRP Publication 116 are given to characterize the operational

325

quantities for directional and individual monitoring. These data sets are also required for the326

calibration and type testing of area monitoring instruments and personal dosimeters. The consistency

327

of numerical values of conversion coefficients to effective dose between ICRP Publication 116 and328

the calculations in this Report to ambient dose and personal dose was studied and validated (Endo,3292017). The numerical values of conversion coefficients to directional and personal absorbed dose to330

the lens of the eye and local skin were carried out using one computer code but were validated by two

331

other codes at a number of discrete energies and angles. The statistical uncertainties in the332

calculations are around 1 % or less.

333

Although the conversion coefficients from fluence or air kerma are to values of protection

334

quantities that are not point quantities but are averaged over an organ or tissue, or the sum of these335

averages, the operational quantities that are recommended are point quantities.

336

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2 Concepts and Terms

337
338
339

2.1

Particle Energy

In this Report, the quantity particle kinetic energy and photon energy, is given the symbol Ep, to340

distinguish the quantity from the quantity effective dose, symbol E.

341

2.2

Charged-Particle Equilibrium

342

Charged-particle equilibrium exists at a point if the distribution of charged-particle radiance

343(Section 3.1.3) with respect to particle energy is constant within distances equal to the charged-

344

particle range. Under condition of charged-particle equilibrium the numerical value of collision345

kerma (Section 3.2.1) at a point of interest approaches the value of absorbed dose (Section 3.2.2).

346

2.3

ICRU 4-Element (soft) Tissue347

ICRU 4-element soft tissue (ICRU, 1980) has a density of 1 g cm-3, and a composition by mass348

of 76.2 % oxygen, 11.1 % carbon, 10.1 % hydrogen, and 2.6 % nitrogen, with no further specification349

of other properties of that material.

350
351
352

2.4

ICRU Sphere

The ICRU sphere (ICRU, 1980) is a 30 cm diameter sphere of ICRU 4-element tissue. The
ICRU sphere is no longer used in the recommended definitions of the operational quantities.

353

2.5

ICRP and ICRU Adult Anthropomorphic Reference Computational Phantoms

354

The anthropomorphic reference computational phantoms of ICRP and ICRU are models of the355

human body presented and described in ICRP Publication 110 (ICRP, 2009), with the anatomical356

and physiological characteristics defined in ICRP Publication 89 (ICRP, 2002). The models are357

represented by arrays of cuboid voxels based on medical tomographic images in which the anatomy358

is described by small three-dimensional volume elements. The collections of these voxels, of a359

number of compositions and densities (ICRP, 2009), are used to specify the organs and tissues of the

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

360

human body. Two reference phantoms have been defined for adults, a male and female one. These

361

generalized body phantoms do not represent any individual human body.

362

2.6

Conversion Coefficients

363

Conversion coefficients relate a protection or operational quantity to a radiometric or364

dosimetric quantity. This term is used in external exposure situations, while in internal dosimetry the365

ratios of dose quantities and activity quantities are called dose coefficients. For external exposure,366

conversion coefficients are given to the operational quantities from the radiometric and dosimetric

367

quantities fluence or air kerma.

368

An internationally agreed set of conversion coefficients for protection quantities is available for369

general use in radiological protection practice for occupational exposures (ICRP, 2010). They are370

calculated for whole-body irradiation of the phantoms in vacuum exposed to broad parallel beams

371

assumed to represent occupational exposure for the field geometries: antero-posterior, (AP), postero-

372

anterior, (PA), left lateral, (LLAT ), right lateral, (RLAT ), rotational, (ROT ), isotropic, (ISO),

373

superior hemisphere semi-isotropic (SS-ISO), inferior hemisphere semi-isotropic (IS-ISO). They are374

available for these ideal exposure geometries only.

375

Conversion coefficients from particle fluence and air kerma to the previously recommended376

operational quantities in well specified exposure conditions were published by ICRU and ICRP

377

(ICRU, 1998; ICRP, 1996). Such data have often been applied for calibration of area monitoring

378

instruments and personal dosimeters used in radiation protection by the ICRU (ICRU, 2001) and the379

International Organization for Standardization, (ISO), (ISO, 1998; 1999; 2006; 2008): these data are

380

replaced by those given in this Report.

381
382

FINAL DRAFT JULY 2017

3 Definitions of Quantities

383
384
385
386
387

NOT TO BE REFERENCED

3.1

Radiometric Quantities

3.1.1 Fluence
The fluence, Φ, (ICRU, 2011) is the quotient of dN by da, where dN is the number of particles
incident on a sphere of cross-sectional area da, thus:

388

Φ

dN
.
da

(3.1)

389

The unit of fluence is m-2.

390

In dosimetric calculations, fluence is frequently expressed in terms of the lengths of the particle

391

trajectories. It can be shown (Weinberg and Wigner, 1958) that the fluence, Φ, is given byΦ = dl/dV,

392
393
394
395

(3.2)

where dl is the sum of the lengths of particle trajectories in the volume dV.
For a radiation field that does not vary over the time interval, t, and is composed of particles
with velocity v, the fluence, Φ, is given by:Φ = n v t,

396

(3.3)

397

where n is the particle number density, given by n = dN/dV, where dN is the number of particles in398

the volume dV.

399

The distributions, ΦEp of the fluence with respect to energy are given by:400ΦEp = dΦ/dEp,

(3.4)

401

where d is the fluence of particles of energy interval between Ep and Ep + dEp. In certain

402

circumstances quantities involving the differential solid angle, dΩ, are required. The complete

403

representation of the double differential of fluence can be written ΦEp,Ω(Ep, Ω).

404

3.1.2 Fluence Rate

FINAL DRAFT JULY 2017

405
406

NOT TO BE REFERENCED

The fluence rate, Φ , (ICRU, 2011) is the quotient of dΦ by dt, where dΦ is the increment of thefluence of particles in the time interval dt, thus:

407

Φ

408

The unit of fluence rate is m-2 s-1.

409

dΦ
.
dt

(3.5)

3.1.3 Particle Radiance410

The particle radiance, Φ Ω , (ICRU, 2011) is the quotient of d Φ by d Ω , where d Φ is the411

fluence rate of particles propagating within a solid angle d Ω around a specified direction, thus:d ΦΦ Ω 
.
dΩ

412
413
414

(3.6)

The unit of particle radiance is m-2 s-1 sr-1. The distribution of particle radiance with respect toenergy is given by:ΦΩ , E 

415

d ΦΩ
,
d Ep

(3.7)

416

where d Φ Ω is the particle radiance for particles of energy between Ep and Ep + dEp. The quantity417ΦΩ , Ep is sometimes termed angular flux or phase flux in radiation-transport theory.

418

Apart from aspects that are of minor importance in the present context (e.g., polarization), the419

field of any radiation of a given particle type is completely specified by the distribution of the particle

420

radiance with respect to particle energy, ΦΩ , Ep , as this defines number, energy, local density, and421

arrival rate of particles propagating in a given direction. This quantity, as well as the distribution of422

the energy radiance with respect to energy, can be considered as basic in radiometry.

423
424

3.2
3.2.1 Kerma

Dosimetric Quantities

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

425

The kerma, K, (ICRU, 2011) for ionizing uncharged particles, is the quotient of dEptr by dm,

426

where dEptr is the mean sum of the initial kinetic energies of all the charged particles liberated in a

427

mass dm of a material by the uncharged particles incident on dm, thus:

428

K

d Ep tr

429

.
(3.8)
dm
The unit of kerma is J kg-l. The special name for the unit of kerma is gray (Gy); 1 Gy = 1 J kg-1.

430

Although kerma is a quantity that concerns the initial transfer of energy to matter, it is431

sometimes used as an approximation to absorbed dose. The numerical value of the kerma approaches

432that of the absorbed dose to the degree that charged-particle equilibrium exists, that radiative losses

433

are negligible, and that the kinetic energy of the uncharged particles is large compared to the binding

434

energy of the liberated charged particles.

435

A quantity related to the kerma, termed the collision kerma, has long been used as an

436

approximation to absorbed dose (Attix, 1979a; 1979b) when radiative losses are not negligible. The

437

collision kerma, Kcol, excludes the radiative losses by the liberated charged particles, and for a438

fluence, Φ, of uncharged particles of energy Ep in a specified material is given by:

Kcol  ΦEp

439

en

 ΦEp tr 1  g   K 1  g 



(3.9)

440

where μen/ρ is the mass energy-absorption coefficient and μtr/ρ is the mass energy-transfer coefficient441

of the material for uncharged particles of energy Ep, and g is the fraction of the total kinetic energy of442

liberated charged particles that would be lost in radiative processes in that material.

443
444

In dosimetric calculations, the collision kerma, Kcol, can be expressed in terms of the
distribution, ΦEp, of the uncharged-particle fluence with respect to energy as:

Kcol   ΦEp Ep

445

en

d Ep   ΦEp Ep tr 1  g  d Ep  K 1  g 

(3.10)

446

where g is the mean value of g averaged over the distribution of the kerma with respect to the447electron energy.

FINAL DRAFT JULY 2017448

NOT TO BE REFERENCED

The kerma rate, K , is the quotient of dK by dt, where dK is the increment of the kerma in the time449

interval dt, thus:

450

K

451

The unit of kerma rate is J kg-1 s-1. The special name for the unit of kerma rate is gray per second

dK
.
dt

452

(Gy s-1).

453

3.2.2 Absorbed Dose

454
455

The absorbed dose, D, (ICRU, 2011) is the quotient of d ε by dm, where d ε is the mean energy
imparted by ionizing radiation to matter of mass dm, thus:
D

456
457
458
459
460

463
464
465
466
467

d
.
dm

(3.12)The unit of absorbed dose is J kg-l. The special name for the unit of absorbed dose is gray (Gy).
3.2.3 Absorbed Dose Rate
The absorbed dose rate, D , (ICRU, 2011) is the quotient of dD by dt, where dD is the incrementof the absorbed dose in the time interval dt, thus:

461

462

(3.11)

dD
D 
.
dt

(3.13)The unit of absorbed dose rate is J kg-1 s-1. The special name for the unit of absorbed dose rate isgray per second (Gy s-1).
3.3

Protection Quantities

3.3.1 Mean Absorbed Dose in an Organ or Tissue
The mean absorbed dose in an organ or tissue T is DT, (ICRP, 2007) defined by:
DT = 1/mT ∫ D dm

(3.14)

468

where mT is the mass of the organ or tissue, and D is the absorbed dose in the mass element dm . The

469

integration extends over the whole organ or tissue.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

470

The unit of mean absorbed dose is joule per kilogram (J kg-1), and its special name is gray (Gy).

471

Two organs or tissues with small or no contribution to effective dose (Section 3.3.3) merit472

attention: the control of the exposure of local skin and the lens of the eye to prevent deterministic473

tissue reactions that occur above a threshold dose.

474

The absorbed dose in local skin is defined as that averaged over 1 cm2 of the skin between

475

depths of 50 µm and 100 µm anywhere on the surface of the body. The composition of skin is given

476

in ICRP Publication 89 (ICRP, 2002), of density 1.09 g cm-3 (ICRP, 2009). The specific annual dose

477

limits recommended for the skin apply to the absorbed dose to local skin at the most highly irradiated478

area of the skin. There has also been increased concern of the effects of irradiation in the lens of the479eye, which has led to a reduction in annual dose limits (ICRP, 2012).

480

3.3.2 Effective Dose

481
482

The weighted sum of absorbed doses in all specified organs and tissues of the body, E, (ICRP,
2007), given by the expression:E   wT  wR DT,R

483

T

(3.15)

R

484

where DT,R is the mean absorbed dose in an organ or tissue T averaged over the male and485

female reference phantoms from radiation of type R, wR is the radiation weighting factor for the486

radiation R incident on the body, and wT is the sex-averaged tissue weighting factor. The sum is487

performed over organs and tissues considered to be sensitive to the induction of stochastic effects.

488

The unit of effective dose is J kg-1. The special name for the unit of effective dose is sievert (Sv).

489
490

3.4

Operational Quantities for External Exposure

3.4.1 Ambient Dose491

The ambient dose, H*, at a point in a radiation field, is the product of the particle fluence at that492

point, Φ, and the conversion coefficient, h*Emax, relating particle fluence to the maximum value of493

effective dose, Emax.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

494

For a given particle type i with kinetic energy Ep, the conversion coefficient h*Emax,i(Ep) =495

Emax,i(Ep)/Φi(Ep,) is calculated for exposure of the whole-body ICRP/ICRU adult reference phantoms

496(ICRP, 2009) for broad parallel beams of the radiation field incident in irradiation geometries AP, PA,

497

LLAT, RLAT, ROT, ISO, SS-ISO, and IS-ISO fields for photons and neutrons; AP, PA, ISO, SS-ISO,

498

and IS-ISO fields for electrons, positrons, muons and pions; and AP, PA, and ISO for He ions (ICRP,

4992010).

500

For a distribution of particles of type i:H*i= ∫ h*Emax,i(Ep) [dΦi(Ep)/dEp] dEp

501( 3.16)502

where dΦi(Ep)/dEp is the fluence of particles with kinetic energies in the interval dEp around Ep. The503

sum over all contributing particle types is:
H* = ∑ H*i

504

The unit of ambient dose is J kg-1. The special name for the unit of ambient dose is sievert (Sv).

505
506

3.4.2 Ambient Dose Rate
The ambient dose rate 𝐻̇ ∗ is the quotient of dH* by dt, where dH*is the increment of the ambient

507
508

(3.17)

dose in the time interval dt, thus:∗d𝐻𝐻̇ ∗ = d𝑡 .

509

(3.18)The unit of ambient dose rate is J kg-l s-1. The special name for the unit of ambient dose rate is

510
511

sievert per second (Sv s-1).

512

3.4.3 Directional Absorbed Dose in the Lens of the Eye

513

The directional absorbed dose in the lens of the eye, D'lens(Ω), at a point in a radiation field with a514

specified direction of incidence, Ω, is the product of the particle fluence at that point, Φ(Ω), and the515

conversion coefficient, d'lens(Ω), relating particle fluence to the value of absorbed dose in the lens of the

516

eye.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

517

For a given particle type i with kinetic energy Ep, the conversion coefficientd'lens,i(Ep,Ω) =518

D'lens,i(Ep,Ω)/Φi(Ep,Ω) is calculated for exposure of the whole-body of the stylized eye model (Behrens

519

and Dietze, 2011) for broad parallel beams of the radiation field incident in the direction Ω. For a given520

Ω, the maximum value of absorbed dose in the lens of the right or left eye is taken.

521

For a distribution of particles of type i:522

D'lens,i(Ω) = ∫ d'lens,i(Ep,Ω) [dΦi(Ep,Ω)/dEp] dEp

523

where dΦi(Ep,Ω)/dEp is the fluence of particles with direction of incidence Ω and with kinetic

524

energies in the interval dEp around Ep. The sum over all contributing particle types i with direction of525

incidence Ω is:D'lens(Ω) = ∑D'lens,i(Ω)

526
527
528

(3.19)(3.20)The unit of directional absorbed dose in the lens of the eye is J kg-1. The special name for theunit of directional absorbed dose in the lens of the eye is gray (Gy).

529

The specification of the incident direction, Ω, requires a reference system for coordinates in which530

the direction of incidence is expressed. This reference system for an area monitoring quantity can be531

related to the radiation field in which the operational quantity is to be determined. In the particular case532

of a unidirectional field, the direction can be related to the angle, α, between this direction and the533

direction of incidence, Ω0, that is antero-posterior, AP, to the stylized eye model. When α = 0º, the value534

of D'lens(Ω) at the point of interest for measurements using this specified direction shall be written D'lens.

535

3.4.4 Directional Absorbed Dose Rate in the Lens of the Eye

536

The directional absorbed dose rate in the lens of the eye, 𝑫′̇lens(Ω), is the quotient of dD'lens(Ω)

537

by dt, where dD'lens(Ω) is the increment of directional absorbed dose in the lens of the eye in the time

538

interval dt, thus:′

539

d𝐷 lens ()𝐷′̇lens (𝛺) =.
d𝑡(3.21)

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

The unit of directional absorbed dose rate in the lens of the eye is J kg-l s-1. The special name

540
541

for the unit of directional absorbed dose rate in the lens of the eye is gray per second (Gy s-1).

542

3.4.5 Directional Absorbed Dose in Local Skin

543

The directional absorbed dose in local skin, D'local skin(Ω), at a point in a radiation field with a544

specified direction of incidence, Ω, is the product of the particle fluence at that point, Φi, and the545

conversion coefficient, d'local skin(Ω), relating particle fluence to the value of absorbed dose in local

546

skin.

547

For a given particle type i with kinetic energy Ep, the conversion coefficient d'local skin,i(Ep,Ω) =548

D'local skin,i(Ep,Ω)/Φ(Ep,Ω) is calculated for exposure to broad parallel beams of the radiation field549

incident in the direction Ω. The conversion coefficient is calculated for exposure of a specified

550

phantom, an ICRU 4-element tissue 300 mm x 300 mm x 150 mm slab (ρ=1.0 g cm-3), in which the551

dose is averaged over the volume of a right circular cylinder between the depths of 50µm and 100 µm

552

and a cross sectional area of 1 cm² below the center of the front surface. Inside the phantom there is553

an outer layer of 2 mm skin of density 1.09 g cm-3 (ICRP, 2009) of elemental composition given in554

ICRP Publication 89 (ICRP, 2002).

555

For a distribution of particles of type i:D'local skin,i(Ω) = ∫ d'local skin,i(Ep,Ω)[dΦi(Ep,Ω))/dEp] dEp

556(3.22)

557

where dΦi(Ep,Ω))/dEp is the fluence of particles with direction of incidence Ω and with kinetic energies

558

in the interval dEp around Ep. The sum over all contributing particle types with direction of incidence Ω

559

is:

560
561
562

D'local skin(Ω) = ∑D'local skin,i(Ω)(3.23)The unit of directional absorbed dose in local skin is J kg-1. The special name for the unit of
directional absorbed dose in local skin is gray (Gy).

563

The specification of the direction of incidence, Ω, requires a reference system for coordinates in564

which the direction is expressed. This reference system for an area monitoring quantity can be related

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

565

to the radiation field in which the operational quantity is to be determined. In the particular case of a566

unidirectional field, the direction can be related to the angle, α, between this direction, and the direction567

of incidence, Ω0, that is normal to the front surface of the slab phantom. When α = 0º, the value of568

D'localskin(Ω) at the point of interest for measurements using this specified direction shall be written D'local

569

skin.

570

3.4.6 Directional Absorbed Dose Rate in Local Skin

571

The directional absorbed dose rate in local skin, 𝑫̇′local skin(Ω), is the quotient of dD'local skin(Ω)

572

by dt, where dD'local skin(Ω) is the increment of the directional absorbed dose to local skin in the time

573

interval dt, thus:
′

d𝐷
()
𝐷′̇local skin (𝛺) = locald𝑡skin .

574

The unit of directional absorbed dose rate in local skin is J kg-l s-1. The special name for the unit

575
576

of directional absorbed dose rate in local skin is gray per second (Gy s-1).

577

3.4.7 Personal Dose

578
579

(3.24)The personal dose, Hp, at a point on the body is the product of the particle fluence incident at thatpoint, Φ, and the conversion coefficient, hp, relating particle fluence to the value of effective dose, E.

580

For a given particle type i with kinetic energy Ep and direction of incidence1 Ω, the conversion

581

coefficient hp,i(Ep,Ω) = E(Ep,Ω)/Φi(Ep,Ω) is calculated for broad parallel beams incident on the whole-582

body ICRP/ICRU adult reference phantoms (ICRP, 2009). For a given Ω, the maximum value of583

effective dose is taken for radiation incident from left or right.

584

For a distribution of particles of type i:
Hp,i= ∫∫ hp,i(Ep,Ω) [dΦi(Ep,Ω)/d EpdΩ] dEpdΩ

585
1(3.25)

A right-handed orthogonal system for the bodyis adopted in which the X-axis is from right to left, the Y-axis from front toback and the Z-axis from toe to head. The irradiation directional angle Ω is defined in terms of the componentsθ and φ, with
θbeing the angle with respect to the Z-axis (positive θpointing to the head) and φ being the projection on to the XY-plane(positive φpointing to the left).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

586

where dΦi(Ep,Ω)/dEpdΩ is the fluence of particles at that point, with kinetic energies in the interval dEp

587

around Ep, and directions of incidence in the interval dΩ around Ω. The sum over all contributing

588

particle types is:
Hp= ∑ Hp,i589

The unit of personal dose is J kg-1. The special name for the unit of personal dose is sievert (Sv).

590
591

(3.26)

3.4.8 Personal Absorbed Dose in the Lens of the Eye

592

The personal absorbed dose in the lens of the eye, Dp lens, at a point on the head or body is the593

product of the particle fluence incident at that point, Φ, and the conversion coefficient, dp lens, relating594

particle fluence to the value of absorbed dose in the lens of the eye.

595

For a given particle type i with kinetic energy Ep and direction of incidence2 Ω, the conversion

596

coefficient dplens,i(Ep,Ω) = Dp lens,i(Ep,Ω)/Φi(Ep,Ω) is calculated for broad parallel beams incident on

597

the whole-body stylized eye model (Behrens and Dietze, 2011). For a given Ω, the maximum value598

of the absorbed doses in the lens of the right or left eye is taken.

599

For a distribution of particles of type i:
Dp lens,i= ∫∫ dp lens,i(Ep,Ω)) [dΦi(Ep,Ω)/dEpdΩ)] dEpdΩ

600(3.27)

601

where dΦi(Ep,Ω)/dEpdΩ is the fluence of particles at that point with kinetic energies in the interval dEp

602

around Ep, and directions of incidence in the interval dΩ around Ω. The sum over all contributing

603

particle types is:
Dp lens = ∑Dplens,i604(3.28)The unit of personal absorbed dose in the lens of the eye is J kg-1. The special name for the unit of

605
606

personal absorbed dose in the lens of the eye is gray (Gy).

607

3.4.9 Personal Absorbed Dose in Local Skin
2

A right-handed orthogonal system for the body is adopted in which the X-axis is from right to left, the Y-axis from front toback and the Z-axis from toe to head. The irradiation directional angle Ω is defined in terms of the componentsθ and φ, with
θbeing the angle with respect to the Z-axis (positive θpointing to the head) and φ being the projection on to the XY-plane(positive φ pointing to the left).[This isthe same asforHp, but different tothatforcalculationsforthe Behrens Dietze model in
ICRP Publication 116]

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

608

The personal absorbed dose in local skin, Dp local skin, is the product of the particle fluence incident609

on the body or extremities, Φ, and the conversion coefficient, dp local skin, relating particle fluence to the610value of absorbed dose in local skin.

611

For a given particle type i with kinetic energy Ep and direction of incidence3 Ω, the conversion

612

coefficient dp local skin,i(Ep,Ω) = Dp local skin,i(Ep,Ω)/Φi(Ep,Ω) is calculated for exposure of the specified

613

phantoms to broad parallel beams:
614

for the trunk, a slab of ICRU 4-element tissue (ρ=1.0 g cm-3) with dimensions 300 mm x

615

300 mm x 150 mm, in which the dose is averaged over the volume of a right circular616

cylinder between the depths of 50 µm and 100 µm and a cross sectional area of 1 cm²

617

below the center of the front surface;618

for the extremities a pillar of ICRU 4-element tissue (ρ=1.11 g cm-3) with dimensions 73

619

mm diameter and 300 mm length, in which the dose is averaged over the volume between

620

the radii 36.4 mm and 36.45 mm with a circle of area 1 cm² projected onto the upper and621

lower cylindrical surfaces perpendicular to and at the center of the pillar;622

for the finger a rod of ICRU 4-element tissue (ρ=1.11 g cm-3) with dimensions 19 mm

623

diameter and 300 mm length, in which the dose is averaged over the volume between the624

radii 9.4 mm and 9.45 mm with a circle of area 1 cm² projected onto the upper and lower625

cylindrical surfaces perpendicular to and at the center of the pillar.

626

Inside each phantom there is an outer layer of 2 mm skin of density 1.09 g cm-3 (ICRP. 2009) with the627elemental composition given in ICRP Publication 89 (2002).

628

For a distribution of particles of type i:
Dp local skin,i= ∫∫ dp local skin,i(Ep,Ω) [dΦi(Ep,Ω)/dEpdΩ] dEpdΩ

629(3.29)

The angle Ω is defined such that the angle θ is the angle of irradiation direction with the axis of the cylinderfor the pillar androd; and the angle θ+ π/2 is the angle of irradiation direction with the normal of the incident radiation surface for the slab;
and φ being the angle of irradiation direction projected onto the plane perpendicular to the cylindrical axis for the pillar androd;and the normal of the incident radiation surface for the slab; with arbitrary direction in this plane for the pillar and rod, as
both are cylindrical symmetric;and with one of the main axis in this planefor the slab.
3

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

630

where dΦi(Ep,Ω)/dEpdΩ is the fluence of particles with kinetic energies in the interval dEp around Ep,

631

and directions of incidence in the interval dΩ around Ω. The sum over all contributing particle types is:

632
633
634
635

Dp local skin = ∑Dp local skin,i(3.30)The unit of personal absorbed dose in local skin is J kg-1. The special name for the unit of
personal absorbed dose in local skin is gray (Gy).

FINAL DRAFT JULY 2017

4 Conversion Coefficients

636
637

NOT TO BE REFERENCED

4.1

Conversion Coefficients for the Operational Quantities

638

The conversion coefficients are calculated for irradiation of the whole-body ICRP/ICRU adult639

reference phantoms (ICRP, 2009) and the phantoms for absorbed dose in the lens of the eye and local

640

skin for broad parallel beams of the radiation field phantoms exposed in vacuo. The specification of the641

incident direction, Ω, requires a reference system for coordinates in which Ω is expressed. For the642

responses of area monitoring instruments to determine directional absorbed dose, this reference system643

can be related to the radiation field. For personal dosimeters to determine personal dose and absorbed

644

dose in the lens of the eye and in local skin, this reference system is related to the body, head and eye,

645

and extremity. In the particular case of a unidirectional field orthogonal to the axis of the whole-body

646

ICRP/ICRU adult reference phantoms from toe to head, or the Z-axis (slab phantom), or the cylinder

647

axis (cylindrical phantoms),the direction of incidence between the direction of the radiation field, Ω, and648

the direction, Ω0, that is antero-posterior to the phantom, is α.

649

In Appendix A, Tables A.1.1a to A.1.10 and Figures A.1.1a to A.1.10 give the numerical values of650

conversion coefficients of ambient dose, H*, (see Section 3.4.1) from fluence for photons, neutrons,

651

electrons, positrons, protons, negative muons, and positive muons, for energies up to 10 GeV; for652

negative pions and positive pions for energies up to 200 GeV; and for He ions up to 100 GeV u-1. Table

653

A.1b and Figure A.1b give the numerical values from air kerma for photons up to 50 MeV.

654

Tables A.2.1a to A.2.10, and Figures A.2.1a to A.2.10 give the numerical values of the655

conversion coefficients from fluence to personal dose, Hp (see Section 3.4.7) for photons, neutrons,

656

electrons, positrons, protons, negative muons, positive muons, negative pions and positive pions for657

energies up to 1GeV; and for He ions up to 1GeV u-1; and in Table A.2.1b and Figure A.2.1b from air

658

kerma for photons up to 50 MeV. The upper energies selected are considered appropriate for personal659

monitoring measurements. Other than for AP, PA, cranial, and caudal incidence, the value of effective

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

660

dose will depend on the angle of incidence, and the conversion coefficients for irradiations in the661

horizontal plane the maximum value of right and left incidences of irradiation is taken. The

662

conversion coefficients are given from 0° (A-P) to 90° in 15°, 180°, and for the irradiation geometries

663

rotational (ROT), isotropic (ISO), superior hemisphere semi-isotropic (SS-ISO), and inferior

664

hemisphere semi-isotropic (IS-ISO).

665

The numerical values of the conversion coefficients from particle fluence to directional absorbed

666

dose in the lens of the eye, D'lens(Ω), (see Section 3.4.3) and personal absorbed dose in the lens of the667eye, Dp lens, (see Section 3.4.8), are the same for the same fluence, particle type, energy, and direction or668

angle of incidence. Tables A.3.1a to A.3.5 and Figures A.3.1a to A.3.5 give the values for photons,

669

neutrons, electrons, positrons, and protons, from fluence, and Table A.3b and Figure A.3b for photons

670

from air kerma for energies up to 50 MeV. The conversion coefficients are given from 0° (A-P) to 90° in

671

15° steps and for a rotational field (ROT).

672

The numerical values of the conversion coefficients of directional absorbed dose in local skin,673

D'local skin(Ω), (see Section 3.4.5), and personal absorbed dose in local skin, Dp local skin, (see Section674

3.4.9), are the same for the 300 mm x 300 mm x 150 mm slab phantom, for the same fluence, particle

675

type, energy, and direction or angle of incidence. Tables A.4.1.1a to A.4.5 and Figures A.4.1.1a to

676

A.4.5 give the values from fluence for photons, neutrons, electrons, positrons, and protons, for677

energies up to 50 MeV; and for alpha particles up to 10 MeV, and table A.4.1b and Figure A.4.1b

678

from air kerma for photons. For directional and personal absorbed dose in local skin for the body, the679

conversion coefficients are given from 0° (A-P) to 75° in 15° steps; for exposure of the extremity and680

finger for angles from 0° to 180° in 15° steps and for a rotational field (ROT).

681

The calibration of area monitoring instruments and personal dosimeters to measure photons for

682

ambient dose, personal dose, directional and personal absorbed dose in the lens of the eye and in local

683

skin, are performed routinely in air with sufficient material in front of the instrument to provide full684

charged-particle equilibrium. The calibration is in terms of air kerma (ISO 29661:2012 (ISO, 2012)).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

685

Appendix A.5 gives values of conversion coefficients of the operational quantities in terms of

686

photon fluence and air kerma for this procedure for energies up to 50 MeV, using the kerma-

687

approximation method in the calculation to approximate charged-particle equilibrium.

688

Appendix B describes the computer codes to calculate the conversion coefficients.

689

Appendix C for information gives conversion coefficients to the operational quantity absorbed

690

dose to the maximum value of the absorbed dose in the complete lens or in the sensitive cells.

691

When a precise interpolation among the values of the conversion coefficients presented in this692

Report is required, it is recommended that a procedure similar to that used in ICRP Publication 116

693(ICRP, 2010) should be followed. For interpolations of the operational quantities per fluence, a four-694

point (cubic) Lagrangian interpolation formula is recommended, and a log–log graph scale is695

appropriate. For interpolations of the operational quantities per air kerma, a linear-log graph scale is696

more appropriate.

697

4.2 Comparison of Values of Recommended and Previous Operational Quantities698

4.2.1 General Remarks

699

In ICRP Publication 116 (ICRP, 2010), the values of the conversion coefficients from fluence to700

the protection quantities for all particles are calculated using full transport of the radiation field. The

701

values of the conversion coefficients of the operational quantity ambient dose equivalent included in702

the figures in ICRP Publication 116 are also calculated using full transport of secondary particles. In

703

ICRU Report 57 (ICRU, 1998) and ICRP Publication 74 (ICRP, 1996), the values of conversion

704

coefficients for H'(10) and Hp(10), H'(0.07) and Hp(0.07) for photons were calculated using the705

kerma- approximation method; ICRU and ICRP note that care must be taken in using these values.

706

The respective ranges of electrons in tissue are 10 mm, 3mm, and 0.07 mm for energies of 2 MeV,

707

740 keV, and 65 keV, Above these energies, conditions for charged-particle equilibrium are not met

708

for calculations of H'(10) and Hp(10), H'(3) and Hp(3), H'(0.07) and Hp(0.07) for irradiation of the

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

709

ICRU sphere or the body in vacuo (Dimbylow and Francis, 1983, 1984; Ferrari and Pelliccioni, 1994,

710

1995; Daure et al., 2011).

711

In some cases conversion coefficients for the current quantities are not available and therefore712

no comparisons are given. For the comparison of conversion coefficients for absorbed dose in the713lens of the eye, values of Hp(3) in a cylindrical phantom are used.

714

The symbols used in these figures are as follows: h* for the fluence to ambient dose conversion

715

coefficient (=H*/), and h*(10) for the value of the previous ambient dose equivalent conversion

716

coefficient (=H*(10)/); hp for the fluence to personal dose conversion coefficient (= Hp/ ) and717

hp(10) for the value of the previous personal dose equivalent conversion coefficient (= Hp(10)/);718

h'lens and hp lens for the fluence to directional and personal absorbed dose in the lens of the eye

719

conversion coefficient (=D'lens/ and =Dp lens/), and h'(3) and hp(3) for the previous fluence to720directional and personal dose equivalent conversion coefficient (=H'(3)/ and =Hp(3); h'local skin and721

hp local skin for the fluence to directional and722

coefficient (=D'local skin/ and =Dp local skin/), and h'(0.07) and hp(0.07) for the previous fluence to723

directional and personal dose equivalent conversion coefficient (=H'(0.07)/ and =Hp(0.07/)).

724

4.2.2 Ambient Dose and Personal Dose

personal absorbed dose in local skin conversion

725

In the following figures, comparisons are given of the numerical values of conversion

726

coefficients of the previous definitions with the recommended values, from particle fluence as a727function of energy of ambient dose for photons, neutrons, electrons, positrons, protons, negative728

muons, positive muons, negative pions, positive pions, and He ions/α particles, and of personal dose729

for photons, neutrons, and electrons.

730
731
732

For higher-energy charged nuclei, Z > 1, the dose equivalent at 10 mm can be an inadequate
estimation of effective dose (see ICRP Publication 123 (ICRP, 2013)).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

733
734
735
736
737
738
739
740
741
742
743
744

Figure 4.1: Comparisons of conversion coefficients for photons of h*(10) PHITS-Endo and h*(10)745

FLUKA-Endo (Endo, 2016b), h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000), and h*(10) (ICRU, 1998)

746

with kerma approximation; with those for h*.

747
748
749
750
751
752
753
754
755
756
757
758
759
760
761
762
763
764
765
766
767
768
769
770
771

Figure 4.2: Comparison of conversion coefficients for photons of hp(10) (Kim and Kim, 1999; Veinot
and Hertel, 2011), and hp(10) ( ICRU, 1998) using the kerma approximation, with those for hp.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

772
773
774
775
776
777
778
779
780
781
782
783
784
785
786
787
788
789
790
791
792
793
794
795

The significant overestimate of effective dose for photons by the previous value of ambient

796

dose equivalent and personal dose equivalent below 100 keV by up to a factor of 5 is because

797

numerical values of dose equivalent at a depth of 10 mm in tissue do not reflect effective dose but

798

were derived to approximately reproduce the maximum dose equivalent in the body, with the799

exception for a small energy region between 20 keV and 100 keV for dose equivalent to endosteal

800

cells. There is a progressive underestimation of effective dose by H*(10) and Hp(10) for photons of801energies above 10 MeV (Pelliccioni, 1998, 2000). The use of the kerma-approximation method in the802

calculation of conversion coefficients in ICRP Publication 74 (ICRP, 1996) and ICRU Report 57

803(ICRU, 1998) allows an agreement of the numerical values of the previous published values of804

ambient and personal dose equivalent in this energy region, with effective dose.

805
806
807
808

Figure 4.3: Comparison of conversion coefficients for photons hp(10,) ( ICRU, 1998) using the
kerma approximation, with those for hp() (Endo, 2017).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

809
810
811
812
813
814
815
816
817
818

819
820

Figure 4.4: Comparisons of conversion coefficients for neutrons of h*(10) PHITS-Endo and h*(10) FLUKA-

821

Endo (Endo, 2016b), h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000), and h*(10) ICRU Report57 (ICRU,

8221998); with those for h*.

823
824
825
826
827
828
829
830
831
832
833
834

835
836

Figure 4.5: Comparisons of conversion coefficients for neutrons of hp(10, ) (ICRU, 1998) with thosefor hp() (Endo, 2017).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

837

The depth of 10 mm in the sphere, or in the body is not the most appropriate to estimate

838

effective dose for neutrons (ICRU, 1985).There are also changes to the ratio from a quantity using

839

quality factor, H*(10) to conversion coefficients based on effective dose that uses radiation weighting

840

factor. There is a progressive underestimation of effective dose by the previous quantity, H*(10), for841

neutrons of energies above 10 MeV.

842

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

843
844
845
846
847
848
849
850
851
852
853
854
855
856
857
858
859
860
861
862

Figure 4.6: Comparisons of conversion coefficients for electrons of h*(10) PHITS-Endo and h*(10) FLUKA-

863

Endo (Endo, 2016b), h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000), and h*(10) ICRU Report 57 (ICRU, 1998);864with those for h*.

865
866
867
868
869
870
871
872
873
874
875
876
877
878
879
880
881
882
883
884

Figure 4.7: Comparison of conversion coefficients for electrons for hp(10, ) ( ICRU, 1998; Grosswendt
and Chartier, 1994) with those for hp() (Endo, 2017).

885

For electrons, the previous quantities, H*(10) and Hp(10), overestimated the recommended

886

quantities between 1 and 10 MeV.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

887

888
889
890
891
892
893
894
895
896
897
898
899
900
901
902
903
904
905

Figure 4.8: Comparisons of conversion coefficients for positrons of h*(10) FLUKA-Endo (Endo, 2016b)

906

and h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000); with those for h*.

907
908
909
910
911
912
913
914
915
916
917
918
919
920
921
922

Figure 4.9: Comparisons of conversion coefficients for protons of h*(10) PHITS-Endo and h*(10) FLUKA-Endo

923(Endo, 2016b), and h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000); with those for h*.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

924
925
926
927
928
929
930
931
932
933
934
935
936
937
938

Figure 4.10: Comparisons of conversion coefficients for negative muons of h*(10) PHITS-Endo and h*(10)939

FLUKA-Endo (Endo, 2016b), and h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000); with those for h*.

940
941
942
943
944
945
946
947
948
949
950
951
952
953
954
955

Figure 4.11: Comparisons of conversion coefficients for positive muons of h*(10) FLUKA-Endo (Endo,956

2016b) and h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000); with those for h*.

957

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

958
959
960
961
962
963
964
965
966
967
968
969
970
971
972

Figure 4.12: Comparisons of conversion coefficients for negative pions of h*(10) PHITS-Endo, h*(10)973

FLUKA-Endo (Endo, 2016b), and h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000); with those for h*.

974
975
976

.

977
978
979
980
981
982
983
984
985
986
987
988

Figure 4.13: Comparisons of conversion coefficients for positive pions of h*(10) FLUKA-Endo (Endo, 2016b)

989

and h*(10) FLUKA-Pelliccioni (Pelliccioni, 2000); with those for h*

990
991

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

992
993
994
995
996
997
998
999
1000
1001
1002
1003
1004
1005
1006
1007

Figure 4.14: Comparisons of conversion coefficients for helium ions of h*(10) PHITS-Endo and h*(10)1008

FLUKA-Endo (Endo, 2016b); with those for h*.

1009
1010

4.2.3

Directional and Personal Absorbed Dose in the Lens of the Eye

1011

For the same fluence, particle type, energy, and direction of incidence, the numerical values of1012

conversion coefficients from particle fluence to directional and personal absorbed dose in the lens of the1013

eye are the same. In the following figures, comparisons are given of the numerical values of conversion

1014

coefficients of the previous definitions, H'(0.07) or Hp(0.07), with the recommended values of the1015

conversion coefficients, d'(α)lens and d(α)p lens, from particle fluence as a function of energy for photons

1016

and electrons.

1017
1018
1019
1020
1021

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1022
1023
1024
1025
1026
1027

1028
1029
1030
1031
1032
1033
1034
1035
1036
1037
1038
1039
1040
1041
1042
1043
1044
1045
1046

Figure 4.15: Comparison of conversion coefficients for photons for h'(3,α) (Behrens, 2017b),with kerma approximation, with those for d'(α)lens (Behrens, 2017a).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1047
1048
1049
1050
1051
1052
1053

1054
1055
1056
1057
1058
1059
1060
1061
1062
1063
1064
1065
1066
1067
1068
1069
1070

1071

Figure 4.16 Comparison of conversion coefficients for photons for hp(3,α) (Gualdrini et al.
2011; Daures et al., 2011), made with kerma approximation, with those for d(α)p lens (Behrens,
2017a) . Data for hp(3,α) are only available from 10keV to 10 MeV.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1072
1073
1074
1075
1076
1077
1078
1079
1080
1081
1082
1083

Figure 4.17 Comparison of conversion coefficients of electrons for hp(3, α) (Ferrari and Gualdrini,2012) with those for dp lens(α), maximum for complete lens of both lenses (Behrens, 2017a).

1084

The Figures show that the numerical values of directional dose equivalent and personal dose1085

equivalent at a depth of 3mm for photons and electrons at certain energies and angles of incidence do

1086

not give a good indication of absorbed dose in the lens of the eye. There is concern in nuclear1087

medicine utilizing beta radiation for the accurate assessment of absorbed dose to the lens of the eye.

1088

4.2.4

Directional and Personal Absorbed Dose in Local Skin1089

For the same fluence, particle type, energy, direction, and specific phantom, the numerical

1090

values of conversion coefficients from particle fluence to directional and personal absorbed dose in1091

local skin are the same. In the following figures, comparisons are given of the of the numerical values

1092

of previous definitions for H'(0.07) or Hp(0.07), with the recommended values of the conversion

1093

coefficients, d'local skin slab() and d'local skin slab(), from particle fluence as a function of energy for1094

photons and electrons.

1095
1096

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1097
1098
1099
1100
1101
1102
1103
1104
1105
1106
1107
1108
1109

Figure 4.18: Comparison of conversion coefficients for photons for h'(0.07, ) using the kerma
approximation ( ICRU, 1998) with those for d'local skin slab() (Daures et al., 2017).

1110
1111
1112
1113
1114
1115
1116
1117
1118
1119
1120
1121

Figure 4.19: Comparison of conversion coefficients for photons for hp(0.07, ) using the kerma
approximation ( ICRU, 1998) with those for dplocal skin slab() (Daures et al., 2017).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1122
1123
1124
1125
1126
1127
1128
1129
1130
1131
1132
1133
1134
1135
1136

Figure 4.20: Comparison of conversion coefficients for electrons for hp(0.07, ) ( ICRU, 1998) withthose for dplocal skin slab() (Daures et al., 2017).

1137

The numerical values of the conversion coefficients given in ICRU Report 57 (ICRU, 1998)

1138

and ICRP Publication 74 (ICRP, 1996) for H'(0.07) and Hp(0.07) for photons above 65 keV using the1139

kerma-approximation method give an overestimation of absorbed dose in local skin, increasing to a1140

factor of 90 for 10 MeV photons (Veinot and Hertel; 2011).

1141
1142
1143
1144
1145
1146
1147
1148
1149

FINAL DRAFT JULY 2017

1150
1151
1152
1153

5
5.1

NOT TO BE REFERENCED

Applications of the Operational Quantities

Operational Quantities and their Application in Occupational Radiation Protection

1154

The role of the operational quantities is to provide an adequate estimate of the protection

1155

quantities in order to assess compliance with the limits and for optimization (see Table 5.1). The

1156

range of particle types and energies given for the protection quantities in ICRP Publication 116 (ICRP

1157

2010) are as follows: photons, neutrons, electrons, positrons, protons, negative muons, and positive1158

muons up to 10 GeV; negative pions and positive pions up to 200 GeV; and He ions up to 1001159

GeV u-1.

1160

Table 5.1: Scheme of operational quantities for dose monitoring in external radiation fields.
Task

Operational quantities forarea monitoring
individual monitoring

Control of effective
dose
Control of doses in thethe lens of the eyeambient dose, H*

personal dose , Hpdirectional absorbed dose in the lensof the eye, D'lens(Ω)

personal absorbed dose in the lensof the eye, Dp lensControl of doses inlocal skin, the hands,
and feetdirectional absorbed dose in local
skin, D'local skin(Ω)

personal absorbed dose in local
skin , Dp local skin1161

In principle, the operational quantities should be defined for all particles and energies for which1162

the protection quantities are provided. Up to now, an internationally agreed data set of conversion

1163

coefficients for operational quantities for monitoring external exposure has been given for photons,

1164

neutrons, and electrons in a restricted energy range. This has been sufficient for the large majority of1165

applications in radiation protection, but more attention is being given to higher energies, and for other1166

types of particles.

1167

The areas of application of operational quantities have increased. The particle types and range1168

of particle energies of the radiation fields used in medical diagnostics and therapy, and scientific1169

research, has been extended. There is the inclusion of natural sources of radiation in ICRP

1170

recommendations: aircraft crews are one of the most highly exposed occupational groups, and the

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1171

radiation field at flight altitudes includes a large component of high-energy particles from cosmic

1172

radiation (ICRU, 2010; ICRP, 2016).

1173

The quantities personal dose, personal absorbed dose in the lens in the eye, and personal

1174

absorbed dose in local skin, are used for retrospective recording in order to show compliance with

1175

regulations in respect of limits, and for optimization.

1176

Operational quantities are measurable. This means that the calibration coefficients of an area

1177

monitoring instrument and personal dosimeter can be determined in terms of an operational quantity1178

in a reference field under reference conditions, where the value of the operational quantity at the1179

point of test is well specified. The calibration coefficients of an area monitoring instrument and1180

personal dosimeter are based on using a reference value of a radiometric or dosimetric quantity,1181

which can be well realized by a standard field quantity at the point of test, and applying a reference

1182

conversion coefficient relating this radiometric or dosimetric quantity to an operational quantity. The

1183

value of the radiometric or dosimetric quantity shall be traceable to a national or international1184

standard. The conversion coefficients for the operational quantities are an integral part of the1185

metrological chain of traceability. In high-energy and complex radiation fields, there are no traceable1186

reference fields to characterize and calibrate instruments.

1187

An area monitoring instrument or a personal dosimeter could be designed for a limited range of1188

particle types, energies and angles of incidence, and this will influence the calibration procedures,

1189

including type-testing, and the routine radiation protection measurement at the workplace.

1190

5.2

Operational Quantities and their Application in Environmental Monitoring

1191

Operational quantities were originally developed for the protection of occupationally exposed

1192

workers. The use of the quantities has been extended to monitoring of radiation exposure of the1193

public from natural and artificial environmental sources of radiation. Applications are radiation

1194

monitoring at the fence of nuclear, medical and other facilities with ambient dosimeters and in

1195

contaminated environments by radionuclides released from such facilities. Radionuclides released

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1196

into the environment deposit on the ground surface, and then migrate into the soil. The migration

1197

behavior of radionuclides in the soil depends on soil types, climate conditions, time after the1198

deposition, and so on. The distribution of radionuclides in the soil influences the radiation field,

1199

energy distribution and angular distribution, above the ground (ICRU, 1994). Operational quantities

1200

play an important role to assess doses for the public under these complex radiation fields.

1201

After the Fukushima Daiichi nuclear power plant accident, a large-scale national environmental

1202

monitoring program has been carried out, and comprehensive data including ambient dose equivalent

1203

rates at 1 m height above the ground surface and radioactivity in the soil have been collected (NRA,1204

2012). Though several kinds of radionuclides were detected by gamma-ray spectrometry of the soil

1205

samples, 137Cs and 134Cs were the significant radionuclides contributing most to the ambient dose1206

equivalent rates. It is important to clarify the relation among radioactivity in the soil, relating the1207

measurement of an area monitoring quantity in air and effective dose for the protection of the public

1208(Saito et al., 2012, 2014; Petoussi-Henss et al., 2012).

1209

FINAL DRAFT JULY 2017

1210

NOT TO BE REFERENCED

6Calibration of Area Monitoring Instruments and Personal Dosimeters

1211

6.1

General1212

The operational quantities for ambient dose, directional absorbed dose in the lens of the eye,1213

and directional absorbed dose in local skin, are for all components of the radiation field in particle

1214

energy and direction at the point of interest, and for personal dose, personal absorbed dose in the lens1215

of the eye, and personal absorbed dose in local skin, for all components of the radiation field in

1216

particle energy and angle of incidence on the body. This can include multiple scattering and nuclear

1217

reactions between the radiation source and the body. Area monitoring instruments and personal1218

dosimeters normally will be specified to determine the contributions for a range of particle energies

1219

and directions and angles of incidence on the body and calibrated for these parameters.

1220

The individual monitoring operational quantity is determined at a point on the body, head, or

1221

extremity, for the fluence or air kerma at that point and a conversion coefficient for broad parallel

1222

fields for this fluence or air kerma incident on the whole-body ICRP/ICRU adult reference phantoms

1223(ICRP, 2009) or the phantoms for absorbed dose in the lens of the eye and local skin. Calibration

1224

procedures can be made to include angles of incidence of fluence or air kerma that are not directly

1225

incident at this point on the body, head, or extremity, using the incident fluence or air kerma at this1226

point: the calibration procedure can be such as to simulate exposure of a person in rotational or

1227

isotropic exposure.

1228

In routine procedures for the calibrations of area monitoring instruments and personal

1229

dosimeters in photon fields, conditions approximating full charged-particle equilibrium are used, and1230

an additional set of conversion coefficients for photons calculated using the kerma-approximation

1231

method is provided (see Appendix A.5) for photon energies up to 50 MeV.

1232

The measurement of H*, generally requires that the radiation field be uniform over the1233

dimensions of the instrument and that the instrument has an isotropic response. The measurement of

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1234

D'lens(Ω) and D'local skin(Ω), also requires that the radiation field be uniform over the dimensions of the1235

instrument and that the instrument has the appropriate response as a function of direction.

1236

No changes are needed in the radiation characteristics, production, and dosimetry of the1237

standard reference fields of ISO, IEC, and BIPM, or in the calibration procedures, but a change to the1238

recommended conversion coefficients for these fields will be required.

1239

6.2 Calibration Phantoms for Personal Dosimeters

1240

The recommended phantoms for the calibration of personal dosimeters for the different

1241
1242

quantities are:


1243
1244

for personal dose: a polymethyl methacrylate (PMMA) 300 mm x 300 mm x 150mm water
filled slab (front wall 2.5 mm thick, other walls 10 mm thick) (ISO, 1999);



for personal absorbed dose in the lens of the eye: a PMMA 200 mm diameter 200 mm length1245

water filled cylinder (cylinder walls and end faces 5 mm thick) (Gualdrini et al. 2011; Daures

1246

et al., 2011; Vanhavere et al., 2012));

1247



for personal absorbed dose in local skin: for the trunk, a PMMA 300 mm x 300 mm x 150mm

1248

water filled slab (ISO, 1999); for the extremity, a PMMA 73 mm diameter 300 mm length water

1249

filled pillar (cylinder walls 2.5 mm thick, end faces 10 mm thick) (ISO, 1999); for the finger, a

1250

PMMA 19 mm diameter 300 mm length rod (ISO, 1999).

1251

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

7

1252

Conclusions

1253

The use of operational quantities based on a value of a radiometric or dosimetric quantity at a

1254

point and a conversion coefficient to a protection quantity has been investigated previously. This

1255

approach is now considered acceptable as the ICRP and ICRU have defined adult reference

1256

computational phantoms for the protection quantities that are widely recognized, and have published1257

conversion coefficients from particle fluence to these quantities. The use of operational quantities that1258

are related directly to the values of the protection quantities simplifies the systems of protection and1259

operational quantities, and assists in the comprehension and consistency of radiation protection

1260

quantities by users.

1261

The recommendations of operational quantities in terms of conversion coefficients to ambient

1262

dose, directional absorbed dose in the lens of the eye, directional absorbed dose in local skin, personal

1263

dose, personal absorbed dose to the lens of the eye, and personal absorbed dose to local skin, are a clean

1264

break from the existing recommendations for operational quantities that are based on dose equivalent in1265

the ICRU 4-element sphere and at a depth in the body, and will give a better estimate of the protection

1266

quantities.

1267

There has been concern that ICRP might make significant changes to the tissue weighting factors

1268

and/or the radiation weighting factors, and this would require revisions of the values of the conversion

1269

coefficients for effective dose. In this were to take place, case, which is expected to be infrequent,1270

changes to the conversion quantities to the operational quantities might then be considered, but would

1271

not be automatic.

1272

The numerical values of conversion coefficients for ambient dose and personal dose for1273

photons of energies from 70 keV to 2 MeV are very close to those given in the current definitions.

1274

The values of these quantities from 2 MeV to 10 MeV, in conditions with full charged-particle

1275

equilibrium when including the contributions to the quantities from the electron conversion

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1276

coefficients, are very close to those given in ICRU Report 57 (ICRU, 1998) and ICRP Publication 74

1277(1996) calculated with the kerma-approximation method. The only changes required for this photon

1278

energy range for the calibration of area monitors and personal dosimeters, are a small change to the1279

instrument constant. The calibration of photon area monitoring instruments and personal dosimeters

1280

are routinely performed under condition of charged particle equilibrium, and conversion coefficients

1281

are given calculated using the kerma-approximation method.

1282

For neutrons, the recommended quantities for ambient dose and personal dose are a1283

considerable improvement on the current values for the determination of the protection quantities.

1284

However, for area monitoring instruments based on the moderation of the neutron fluence, no1285

changes are required initially for workplace fields.

1286

Modifications of existing instrumentation might be required where this is considered to be1287

necessary:

1288



1289

for photon energies below 70 keV, to correct for the large overestimation of effective doseby current area monitors and personal dosimeters;

1290



to improve the estimation for photons and electrons of absorbed dose in the lens of the eye;

1291



to determine for photons with energies between 2 MeV and 10 MeV for ambient and

1292

personal dose, if charged-particle equilibrium is not present, but this will depend on the1293

detector system;

1294



to improve the performance of area monitoring instruments and dosimeters for neutron

1295

energies from thermal to 2 MeV in order to correct for the lower value of the conversion

1296

coefficients from particle fluence to H* and Hp compared to H*(10) and Hp(10), and to1297

improve the response above neutrons of energy of 50 MeV in order to correct for the1298higher value.

1299
1300

The recommended operational quantities will provide a solution to the protection problems inradiation fields of higher-energy photons, electrons and neutrons, and for other particle types.

FINAL DRAFT JULY 2017

1

NOT TO BE REFERENCED

Report No. XX

2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41

OPERATIONAL QUANTITIES FOR
EXTERNAL RADIATION EXPOSURE

THE INTERNATIONAL COMMISSION ON
RADIATION UNITS AND
MEASUREMENTS
andTHE INTERNATIONAL COMMISSION ON
RADIOLOGICAL PROTECTIONMONTH 2017

Journal of the ICRU Volume XX No X 2017
ISBN XXXXXXXXXX
Published by Oxford University Press

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

42
43
44
45
46

OPERATIONAL QUANTITIES FOR
EXTERNAL RADIATION EXPOSURE

47
48
49
50
51
52
53
54
55
56
57
58

Report Committee

59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82

N.E.Hertel (Co-Chair), Georgia Institute of Technology, USA.
D.T. Bartlett (Co-Chair), Abingdon, UK
R.Behrens, Physikalisch-Technische Bundesanstalt, Braunschweig, Germany
J-M.Bordy, CEA, LIST, Laboratoire National Henri Becquerel (LNE-LNHB), 91191 Gif-sur-Yvette,
France†G..Dietze , Braunschweig, Germany
A. Endo, Japan Atomic Energy Agency, Japan
G.Gualdrini, Ente per le Nuove Tecnologie, L’Energia e L’Ambiente, Bologna, Italy (until 2015)
T. Otto, European Organization for Nuclear Research (CERN), Geneva, Switzerland
M.Pelliccioni, Istituto Nazionale di Fisica Nucleare, Frascati, Italy

Consultants to the Report Committee
P. Ambrosi, Physikalisch-Technische Bundesanstalt, Braunschweig, Germany (until 2014)
M.B.Bellamy, Center for Radiation Protection Knowledge, Oak Ridge National Laboratory, Oak Ridge,
USA
J-F. Bottollier-Depois, Institut de Radioprotection et de Sûreté Nucléaire,
Fontenay-aux-Roses, France
J. Daures, CEA, LIST, Laboratoire National Henri Becquerel (LNE-LNHB), 91191 Gif-sur-Yvette,
FranceK.F. Eckerman, Oak Ridge,USA
P. Ferrari, Ente per le Nuove Tecnologie, L’Energia e L’Ambiente, Bologna, Italy
B.R.L. Siebert, Braunschweig, Germany
K.G. Veinot, Y-12 National Security Complex, Oak Ridge, Tennessee, USA

ICRU Sponsors
D.T. Burns, Bureau International des Poids et Mesures, Sèvres, France
E. Fantuzzi, Ente per le Nuove Tecnologie, L’Energia e L’Ambiente, Bologna, Italy
H-G. Menzel, Heidelberg, Germany†

Deceased. Dr Dietze played an important role in thedevelepment of the recommendations of thisReport. The Commission wishes to acknowledge
the loss resulting from his untimely death on 25th
January 2015 .

FINAL DRAFT JULY 2017

Appendix A

83
84
85

NOT TO BE REFERENCED

Values of conversion coefficients
A.1

Ambient Dose86

Tables A.1.1a to A.1.10 and Figures A.1.1a to A.1.10 give the values of conversion coefficients,

87

h*Emax, from particle fluence to ambient dose for photons, neutrons, electrons, positrons, protons,

88

negative muons, and positive muons for energies up to 10 GeV; for negative pions and positive pions

89

for energies up to 200 GeV; and for He ions up to 100 GeV u-1. The conversion coefficients relate the90particle fluence to the maximum value of the effective dose, Emax, calculated for whole-body

91

exposure of the ICRP/ICRU adult reference

92

incident in irradiation geometries AP, PA, LLAT, RLAT, ROT, ISO, SS-ISO, and IS-ISO fields for93

photons and neutrons; AP, PA, ISO, SS-ISO, and IS-ISO fields for electrons, positrons, muons and94

pions; and AP, PA, and ISO for He ions (ICRP, 2010). For photons of energy up to 50 MeV, Table

95

A.1.1b and Figure A.1.1b give conversion coefficients from air kerma.

96

phantoms (ICRP, 2009) for broad parallel beams

FINAL DRAFT JULY 201797

Table A.1.1a Conversion coefficients from photon fluence to ambient dose (ICRP, 2010; Endo 2016b).
Ep / MeV
5.000E-03
6.000E-03
7.000E-03
8.000E-03
9.000E-03
1.000E-02
1.200E-02
1.300E-02
1.500E-02
1.700E-02
2.000E-02
2.500E-02
3.000E-02
4.000E-02
5.000E-02
6.000E-02
7.000E-02
8.000E-02
1.000E-01
1.500E-01
2.000E-01
3.000E-01
4.000E-01
5.000E-01
5.110E-01
6.000E-01
6.620E-01
8.000E-01
1.000E+00
1.117E+00
1.330E+00
1.500E+00

98
99
100
101
102
103
104

NOT TO BE REFERENCED

h*Emax/ (pSv cm2)
1.34E-02
1.66E-02
2.25E-02
3.35E-02
4.90E-02
6.85E-02
1.05E-01
1.22E-01
1.56E-01
1.81E-01
2.25E-01
2.75E-01
3.12E-01
3.50E-01
3.69E-01
3.89E-01
4.11E-01
4.43E-01
5.18E-01
7.47E-01
1.00E+00
1.51E+00
2.00E+00
2.47E+00
2.52E+00
2.91E+00
3.17E+00
3.73E+00
4.49E+00
4.90E+00
5.60E+00
6.12E+00

Ep / MeV
2.000E+00
3.000E+00
4.000E+00
5.000E+00
6.000E+00
6.129E+00
8.000E+00
1.000E+01
1.500E+01
2.000E+01
3.000E+01
4.000E+01
5.000E+01
6.000E+01
8.000E+01
1.000E+02
1.500E+02
2.000E+02
3.000E+02
4.000E+02
5.000E+02
6.000E+02
8.000E+02
1.000E+03
1.500E+03
2.000E+03
3.000E+03
4.000E+03
5.000E+03
6.000E+03
8.000E+03
1.000E+04

h*Emax/ (pSv cm2)
7.48E+00
9.75E+00
1.17E+01
1.34E+01
1.50E+01
1.52E+01
1.86E+01
2.21E+01
3.04E+01
3.82E+01
5.13E+01
6.18E+01
7.23E+01
8.21E+01
9.81E+01
1.10E+02
1.30E+02
1.44E+02
1.61E+02
1.73E+02
1.81E+02
1.87E+02
1.96E+02
2.06E+02
2.13E+02
2.36E+02
2.53E+02
2.67E+02
2.77E+02
2.85E+02
2.99E+02
3.07E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120

Figure A.1.1a Conversion coefficients from photon fluence to ambient dose (ICRP, 2010; Endo
2016b).

FINAL DRAFT JULY 2017

121
122

Table A.1.1b Conversion coefficients from photon air kerma to ambient dose (ICRP, 2010; Endo
2016b).
Ep / MeV
5.000E-03
6.000E-03
7.000E-03
8.000E-03
9.000E-03
1.000E-02
1.200E-02
1.300E-02
1.500E-02
1.700E-02
2.000E-02
2.500E-02
3.000E-02
4.000E-02
5.000E-02
6.000E-02
7.000E-02
8.000E-02
1.000E-01
1.500E-01
2.000E-01
3.000E-01
4.000E-01

123
124

NOT TO BE REFERENCED

h*Emax/ (Sv Gy-1)
4.37E-04
7.81E-04
1.45E-03
2.84E-03
5.31E-03
9.26E-03
2.09E-02
2.88E-02
4.99E-02
7.58E-02
1.34E-01
2.60E-01
4.32E-01
8.16E-01
1.14E+00
1.35E+00
1.43E+00
1.44E+00
1.39E+00
1.25E+00
1.17E+00
1.09E+00
1.06E+00

Ep / MeV
5.000E-01
5.110E-01
6.000E-01
6.620E-01
8.000E-01
1.000E+00
1.117E+00
1.330E+00
1.500E+00
2.000E+00
3.000E+00
4.000E+00
5.000E+00
6.000E+00
6.129E+00
8.000E+00
1.000E+01
1.500E+01
2.000E+01
3.000E+01
4.000E+01
5.000E+01

h*Emax/ (Sv Gy-1)
1.04E+00
1.04E+00
1.02E+00
1.02E+00
1.01E+00
1.00E+00
1.00E+00
1.00E+00
9.96E-01
9.90E-01
9.77E-01
9.64E-01
9.45E-01
9.28E-01
9.25E-01
9.24E-01
9.16E-01
8.82E-01
8.42E-01
7.48E-01
6.62E-01
6.07E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141

Figure A.1.1b Conversion coefficients from photon air kerma to ambient dose (ICRP, 2010; Endo
2016b).

FINAL DRAFT JULY 2017142

Table A.1.2 Conversion coefficients from neutron fluence to ambient dose (ICRP, 2010).
Ep / MeV
1.00E-09
1.00E-08
2.50E-08
1.00E-07
2.00E-07
5.00E-07
1.00E-06
2.00E-06
5.00E-06
1.00E-05
2.00E-05
5.00E-05
1.00E-04
2.00E-04
5.00E-04
1.00E-03
2.00E-03
5.00E-03
1.00E-02
2.00E-02
3.00E-02
5.00E-02
7.00E-02
1.00E-01
1.50E-01
2.00E-01
3.00E-01
5.00E-01
7.00E-01
9.00E-01
1.00E+00
1.20E+00
1.50E+00
2.00E+00

143
144
145
146
147
148

NOT TO BE REFERENCED

h*Emax/ (pSv cm2)
3.09E+00
3.55E+00
4.00E+00
5.20E+00
5.87E+00
6.59E+00
7.03E+00
7.39E+00
7.71E+00
7.82E+00
7.84E+00
7.82E+00
7.79E+00
7.73E+00
7.54E+00
7.54E+00
7.61E+00
7.97E+00
9.11E+00
1.22E+01
1.57E+01
2.30E+01
3.06E+01
4.19E+01
6.06E+01
7.88E+01
1.14E+02
1.77E+02
2.32E+02
2.79E+02
3.01E+02
3.30E+02
3.65E+02
4.07E+02

Ep / MeV
3.00E+00
4.00E+00
5.00E+00
6.00E+00
7.00E+00
8.00E+00
9.00E+00
1.00E+01
1.20E+01
1.40E+01
1.50E+01
1.60E+01
1.80E+01
2.00E+01
2.10E+01
3.00E+01
5.00E+01
7.50E+01
1.00E+02
1.30E+02
1.50E+02
1.80E+02
2.00E+02
3.00E+02
4.00E+02
5.00E+02
6.00E+02
7.00E+02
8.00E+02
9.00E+02
1.00E+03
2.00E+03
5.00E+03
1.00E+04

h*Emax/ (pSv cm2)
4.58E+02
4.83E+02
4.94E+02
4.98E+02
4.99E+02
4.99E+02
5.00E+02
5.00E+02
4.99E+02
4.95E+02
4.93E+02
4.90E+02
4.84E+02
4.77E+02
4.74E+02
4.53E+02
4.33E+02
4.39E+02
4.44E+02
4.46E+02
4.46E+02
4.47E+02
4.48E+02
4.73E+02
5.15E+02
5.33E+02
5.69E+02
6.25E+02
6.38E+02
6.45E+02
6.63E+02
7.69E+02
1.04E+03
1.39E+03

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173

Figure A.1.2 Conversion coefficients from neutron fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017174

Table A.1.3 Conversion coefficients from electron fluence to ambient dose (ICRP, 2010).
Ep / MeV
1.00E-02
1.50E-02
2.00E-02
3.00E-02
4.00E-02
5.00E-02
6.00E-02
8.00E-02
1.00E-01
1.50E-01
2.00E-01
3.00E-01
4.00E-01
5.00E-01
6.00E-01
8.00E-01
1.00E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
8.00E+00
1.00E+01

175
176
177
178
179
180
181
182
183
184

NOT TO BE REFERENCED

h*Emax/ (pSv cm2)
2.69E-02
4.04E-02
5.39E-02
8.10E-02
1.08E-01
1.35E-01
1.63E-01
2.18E-01
2.75E-01
4.18E-01
5.69E-01
8.89E-01
1.24E+00
1.63E+00
2.05E+00
4.04E+00
7.10E+00
1.50E+01
2.24E+01
3.61E+01
4.82E+01
5.93E+01
7.06E+01
9.79E+01
1.25E+02

Ep / MeV
1.50E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01
6.00E+01
8.00E+01
1.00E+02
1.50E+02
2.00E+02
3.00E+02
4.00E+02
5.00E+02
6.00E+02
8.00E+02
1.00E+03
1.50E+03
2.00E+03
3.00E+03
4.00E+03
5.00E+03
6.00E+03
8.00E+03
1.00E+04

h*Emax/ (pSv cm2)
1.88E+02
2.36E+02
3.02E+02
3.29E+02
3.37E+02
3.44E+02
3.58E+02
3.66E+02
3.79E+02
3.88E+02
4.11E+02
4.35E+02
4.49E+02
4.64E+02
4.88E+02
5.08E+02
5.25E+02
5.68E+02
6.08E+02
6.38E+02
6.61E+02
6.83E+02
7.16E+02
7.42E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200

Figure A.1.3 Conversion coefficients from electron fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017

201

Table A.1.4 Conversion coefficients from positron fluence to ambient dose (ICRP, 2010).
Ep / MeV
1.00E-02
1.50E-02
2.00E-02
3.00E-02
4.00E-02
5.00E-02
6.00E-02
8.00E-02
1.00E-01
1.50E-01
2.00E-01
3.00E-01
4.00E-01
5.00E-01
6.00E-01
8.00E-01
1.00E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
8.00E+00
1.00E+01

202
203
204
205
206
207
208
209
210
211

NOT TO BE REFERENCED

h*Emax/ (pSv cm2)
3.28E+00
3.29E+00
3.30E+00
3.33E+00
3.36E+00
3.39E+00
3.42E+00
3.47E+00
3.53E+00
3.67E+00
3.84E+00
4.16E+00
4.52E+00
4.90E+00
5.36E+00
7.41E+00
1.05E+01
1.83E+01
2.57E+01
3.91E+01
5.10E+01
6.17E+01
7.29E+01
9.90E+01
1.26E+02

Ep / MeV
1.50E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01
6.00E+01
8.00E+01
1.00E+02
1.50E+02
2.00E+02
3.00E+02
4.00E+02
5.00E+02
6.00E+02
8.00E+02
1.00E+03
1.50E+03
2.00E+03
3.00E+03
4.00E+03
5.00E+03
6.00E+03
8.00E+03
1.00E+04

h*Emax/ (pSv cm2)
1.84E+02
2.29E+02
2.94E+02
3.20E+02
3.27E+02
3.34E+02
3.49E+02
3.57E+02
3.71E+02
3.83E+02
4.12E+02
4.35E+02
4.49E+02
4.62E+02
4.85E+02
5.05E+02
5.22E+02
5.66E+02
6.04E+02
6.33E+02
6.59E+02
6.83E+02
7.16E+02
7.46E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

212
213
214
215
216
217
218
219
220
221
222
223
224
225
226
227
228

Figure A.1.4 Conversion coefficients from positron fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017229

NOT TO BE REFERENCED

Table A.1.5 Conversion coefficients from proton fluence to ambient dose (ICRP, 2010).
Ep / MeV
1.00E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
8.00E+00
1.00E+01
1.50E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01
6.00E+01
8.00E+01
1.00E+02
1.50E+02
2.00E+02
3.00E+02
4.00E+02
5.00E+02
6.00E+02
8.00E+02
1.00E+03
1.50E+03
2.00E+03
3.00E+03
4.00E+03
5.00E+03
6.00E+03
8.00E+03
1.00E+04

230
231
232
233
234
235

h*Emax/ (pSv cm2)
5.47E+00
8.21E+00
1.09E+01
1.64E+01
2.19E+01
2.73E+01
3.28E+01
4.37E+01
5.49E+01
1.89E+02
4.28E+02
7.50E+02
1.02E+03
1.18E+03
1.48E+03
2.16E+03
2.51E+03
2.82E+03
2.18E+03
1.45E+03
1.30E+03
1.24E+03
1.23E+03
1.23E+03
1.23E+03
1.25E+03
1.28E+03
1.35E+03
1.48E+03
1.46E+03
1.71E+03
1.88E+03
1.93E+03

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

236
237
238
239
240
241
242
243
244
245
246
247
248
249
250

Figure A.1.5 Conversion coefficients from proton fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017251

NOT TO BE REFERENCED

Table A.1.6 Conversion coefficients from negative muon fluence to ambient dose (ICRP, 2010).
Ep / MeV
1.00E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
8.00E+00
1.00E+01
1.50E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01
6.00E+01
8.00E+01
1.00E+02
1.50E+02
2.00E+02
3.00E+02
4.00E+02
5.00E+02
6.00E+02
8.00E+02
1.00E+03
1.50E+03
2.00E+03
3.00E+03
4.00E+03
5.00E+03
6.00E+03
8.00E+03
1.00E+04

252
253
254
255
256
257

h*Emax/ (pSv cm2)
1.80E+02
1.80E+02
1.84E+02
1.88E+02
1.93E+02
2.05E+02
2.42E+02
2.93E+02
3.32E+02
4.14E+02
4.65E+02
6.57E+02
7.35E+02
7.55E+02
7.75E+02
5.05E+02
4.35E+02
3.55E+02
3.33E+02
3.22E+02
3.22E+02
3.24E+02
3.28E+02
3.33E+02
3.42E+02
3.38E+02
3.41E+02
3.44E+02
3.47E+02
3.48E+02
3.47E+02
3.49E+02
3.49E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

258
259
260
261
262
263
264
265
266
267
268
269
270
271
272

Figure A.1.6 Conversion coefficients from negative muon fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017273

NOT TO BE REFERENCED

Table A.1.7 Conversion coefficients from positive muon fluence to ambient dose (ICRP, 2010).

274
Ep / MeV
1.00E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
8.00E+00
1.00E+01
1.50E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01
6.00E+01
8.00E+01
1.00E+02
1.50E+02
2.00E+02
3.00E+02
4.00E+02
5.00E+02
6.00E+02
8.00E+02
1.00E+03
1.50E+03
2.00E+03
3.00E+03
4.00E+03
5.00E+03
6.00E+03
8.00E+03
1.00E+04

275
276
277
278
279

h*Emax/ (pSv cm2)
1.94E+02
1.96E+02
1.98E+02
2.02E+02
2.07E+02
2.16E+02
2.51E+02
3.00E+02
3.40E+02
4.25E+02
4.81E+02
6.74E+02
7.51E+02
7.68E+02
7.87E+02
5.10E+02
4.37E+02
3.54E+02
3.33E+02
3.20E+02
3.21E+02
3.23E+02
3.25E+02
3.30E+02
3.34E+02
3.39E+02
3.41E+02
3.44E+02
3.47E+02
3.48E+02
3.47E+02
3.49E+02
3.49E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

280
281
282
283
284
285
286
287
288
289
290
291
292
293
294

Figure A.1.7 Conversion coefficients from positive muon fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017

295

Table A.1.8 Conversion coefficients from negative pion fluence to ambient dose (ICRP, 2010).
Ep / MeV
1.00E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
8.00E+00
1.00E+01
1.50E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01
6.00E+01
8.00E+01
1.00E+02
1.50E+02
2.00E+02
3.00E+02
4.00E+02
5.00E+02

296
297
298
299
300
301
302
303
304
305
306
307

NOT TO BE REFERENCED

h*Emax/ (pSv cm2)
4.06E+02
4.22E+02
4.33E+02
4.58E+02
4.91E+02
5.28E+02
6.73E+02
9.65E+02
1.09E+03
1.25E+03
1.28E+03
1.77E+03
1.92E+03
1.93E+03
1.99E+03
1.31E+03
1.03E+03
9.27E+02
9.02E+02
8.48E+02
8.50E+02
8.80E+02

Ep / MeV
6.00E+02
8.00E+02
1.00E+03
1.50E+03
2.00E+03
3.00E+03
4.00E+03
5.00E+03
6.00E+03
8.00E+03
1.00E+04
1.50E+04
2.00E+04
3.00E+04
4.00E+04
5.00E+04
6.00E+04
8.00E+04
1.00E+05
1.50E+05
2.00E+05

h*Emax/ (pSv cm2)
9.17E+02
9.76E+02
1.02E+03
1.08E+03
1.12E+03
1.13E+03
1.17E+03
1.23E+03
1.26E+03
1.39E+03
1.46E+03
1.60E+03
1.70E+03
1.86E+03
1.99E+03
2.11E+03
2.21E+03
2.42E+03
2.60E+03
2.98E+03
3.14E+03

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

308
309
310
311
312
313
314
315
316
317
318
319
320
321

Figure A.1.8 Conversion coefficients from negative pion fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017

322

Table A.1.9 Conversion coefficients from positive pion fluence to ambient dose (ICRP, 2010).
Ep / MeV
1.00E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
8.00E+00
1.00E+01
1.50E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01
6.00E+01
8.00E+01
1.00E+02
1.50E+02
2.00E+02
3.00E+02
4.00E+02
5.00E+02

323
324
325
326
327
328
329
330
331
332
333
334

NOT TO BE REFERENCED

h*Emax/ (pSv cm2)
3.14E+02
3.24E+02
3.40E+02
3.79E+02
4.29E+02
4.89E+02
5.40E+02
7.17E+02
8.19E+02
1.00E+03
1.10E+03
1.52E+03
1.75E+03
1.83E+03
1.82E+03
1.38E+03
1.13E+03
1.22E+03
1.25E+03
1.10E+03
9.98E+02
9.70E+02

Ep / MeV
6.00E+02
8.00E+02
1.00E+03
1.50E+03
2.00E+03
3.00E+03
4.00E+03
5.00E+03
6.00E+03
8.00E+03
1.00E+04
1.50E+04
2.00E+04
3.00E+04
4.00E+04
5.00E+04
6.00E+04
8.00E+04
1.00E+05
1.50E+05
2.00E+05

h*Emax/ (pSv cm2)
9.80E+02
1.04E+03
1.09E+03
1.16E+03
1.19E+03
1.18E+03
1.21E+03
1.27E+03
1.29E+03
1.39E+03
1.46E+03
1.60E+03
1.69E+03
1.86E+03
1.97E+03
2.09E+03
2.20E+03
2.38E+03
2.53E+03
2.90E+03
3.24E+03

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

335
336
337
338
339
340
341
342
343
344
345
346
347
348
349

Figure A.1.9 Conversion coefficients from positive pion fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017350

NOT TO BE REFERENCED

Table A.1.10 Conversion coefficients from He ion fluence to ambient dose (ICRP, 2010).
Ep / MeV u-1
1.00E+00
2.00E+00
3.00E+00
5.00E+00
1.00E+01
1.40E+01
2.00E+01
3.00E+01
5.00E+01
7.50E+01
1.00E+02
1.50E+02
2.00E+02
3.00E+02
5.00E+02
7.00E+02
1.00E+03
2.00E+03
3.00E+03
5.00E+03
1.00E+04
2.00E+04
5.00E+04
1.00E+05

351
352
353
354
355
356
357
358
359
360
361

h*Emax/ (pSv cm2)
2.19E+02
4.38E+02
6.57E+02
1.09E+03
2.19E+03
4.61E+03
1.72E+04
3.01E+04
4.75E+04
8.05E+04
1.01E+05
1.10E+05
7.29E+04
5.33E+04
4.49E+04
4.60E+04
4.47E+04
4.80E+04
5.01E+04
5.17E+04
6.26E+04
7.10E+04
9.67E+04
1.24E+05

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

362
363
364
365
366
367
368
369
370
371
372
373
374
375

Figure A.1.10 Conversion coefficients from He ion fluence to ambient dose (ICRP, 2010).

FINAL DRAFT JULY 2017

376

A.2

NOT TO BE REFERENCED

Personal Dose

377

Tables A.2.1 to A.2.10 and Figures A.2.1 to A.2.10 give the values of conversion coefficients from378

particle fluence to personal dose for photons, neutrons, electrons, positrons, protons, negative muons,379

positive muons, negative pions and positive pions for energies up to 1GeV, and for He ions up to 1GeV380

u-1. The conversion coefficients relate the particle fluence to effective dose, E, calculated for whole-381

body exposure of the ICRP/ICRU adult reference phantoms (ICRP, 2009) for broad parallel beams

382

incident at angles of incidence from 0° (A-P) to 90° in 15° steps, the maximum value of right or left

383

irradiations is taken, 180°, rotational, isotropic, superior hemisphere semi-isotropic, and inferior

384

hemisphere semi-isotropic fields.

ℎp (𝛼) =

385

𝐸(𝛼)
𝛷(𝛼)

386
387
388
389
390
391
392
393
394
395
396
397

Definition of the incident angle  for parallel beam irradiation: the origin of the coordinate system islocated at the center of the human body.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

398
399

The conversion coefficients of Tables A.2.1a to A.2.10 and Figures A.2.1a to A.2.10 are compiled

400

from those given in ICRP Publication 116 (ICRP, 2010) and from calculations by Endo (2016b, 2017).

401

ICRP Publication 116 provides conversion coefficients for broad parallel and isotropic beams of the402

radiation field at that point incident in irradiation geometries AP, PA, LLAT, RLAT, ROT, ISO, SS-ISO,403

and IS-ISO fields for photons and neutrons; AP, PA, ISO, SS-ISO, and IS-ISO fields for electrons,

404

positrons, muons and pions; and AP, PA, and ISO for He ions. For photons of energy up to 50 MeV,

405

Table A.4.1b and Figure A.4.1b give conversion coefficients from air kerma.

406

The AP, PA, LLAT and RLAT corresponds to  = 0, 180, -90 and +90, respectively, of hp(), and407

these conversion coefficients from ICRP Publication 116 are used in Tables A.2.1a/b A.2.10 and Figures408

A.2.1a/b to A.2.10. The conversion coefficients for incident geometries not available from ICRP

409

Publication 116 are taken from the calculations by Endo (2016b, 2017). The consistency of numerical

410

values between ICRP Publication 116 and the calculations by Endo was studied and validated (Endo,4112017).

412
413

FINAL DRAFT JULY 2017

414
415

NOT TO BE REFERENCED

Table A.2.1a Conversion coefficients from photon fluence to personal dose (ICRP, 2010; Endo, 2016b,
2017).
hp() / (pSv cm2)
Ep / MeV
5.0E-03
6.0E-03
7.0E-038.0E-03
9.0E-03
1.0E-02
1.2E-02
1.3E-02
1.5E-02
1.7E-022.0E-02
2.5E-02
3.0E-02
4.0E-02
5.0E-02
6.0E-02
7.0E-028.0E-02
1.0E-01
1.5E-01
2.0E-01
3.0E-01
4.0E-01
5.0E-01
6.0E-01
8.0E-01
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01
6.0E+01
8.0E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
8.0E+02
1.0E+03

416
417
418
419
420

0
1.34E-02
1.66E-02
2.25E-02
3.35E-02
4.90E-02
6.85E-02
1.05E-01
1.22E-01
1.56E-01
1.81E-01
2.25E-01
2.75E-01
3.12E-01
3.50E-01
3.69E-01
3.89E-01
4.11E-01
4.43E-01
5.18E-01
7.47E-01
1.00E+00
1.51E+00
2.00E+00
2.47E+00
2.91E+00
3.73E+00
4.49E+00
6.12E+00
7.48E+00
9.75E+00
1.17E+01
1.34E+01
1.50E+01
1.78E+01
2.05E+01
2.61E+01
3.08E+01
3.79E+01
4.32E+01
4.71E+01
5.01E+01
5.45E+01
5.78E+01
6.32E+01
6.72E+01
7.23E+01
7.54E+01
7.74E+01
7.87E+01
8.04E+01
8.16E+01

max(15) max(30) max(45) max(60) max(75) max(90)
1.41E-02
1.80E-02
2.45E-02
3.51E-02
5.01E-02
6.77E-02
1.04E-01
1.21E-01
1.52E-01
1.80E-01
2.19E-01
2.71E-01
3.07E-01
3.43E-01
3.62E-01
3.85E-01
4.12E-01
4.38E-01
5.15E-01
7.52E-01
1.00E+00
1.51E+00
2.00E+00
2.47E+00
2.93E+00
3.75E+00
4.55E+00
6.17E+00
7.53E+00
9.84E+00
1.17E+01
1.34E+01
1.51E+01
1.80E+01
2.06E+01
2.65E+01
3.10E+01
3.84E+01
4.36E+01
4.74E+01
5.15E+01
5.63E+01
5.97E+01
6.47E+01
6.86E+01
7.47E+01
7.88E+01
7.97E+01
8.11E+01
8.26E+01
8.40E+01

1.39E-02
1.82E-02
2.45E-02
3.41E-02
4.70E-02
6.23E-02
9.53E-02
1.11E-01
1.40E-01
1.68E-01
2.05E-01
2.57E-01
2.93E-01
3.31E-01
3.53E-01
3.67E-01
3.92E-01
4.21E-01
4.90E-01
7.18E-01
9.68E-01
1.46E+00
1.94E+00
2.40E+00
2.85E+00
3.66E+00
4.42E+00
6.06E+00
7.41E+00
9.66E+00
1.16E+01
1.33E+01
1.49E+01
1.81E+01
2.08E+01
2.65E+01
3.14E+01
3.87E+01
4.49E+01
4.89E+01
5.40E+01
5.87E+01
6.22E+01
6.80E+01
7.23E+01
7.79E+01
8.21E+01
8.37E+01
8.49E+01
8.74E+01
8.94E+01

1.31E-02
1.72E-02
2.28E-02
3.07E-02
4.09E-02
5.31E-02
8.00E-02
9.37E-02
1.19E-01
1.44E-01
1.81E-01
2.32E-01
2.62E-01
2.96E-01
3.14E-01
3.30E-01
3.53E-01
3.81E-01
4.56E-01
6.63E-01
9.01E-01
1.38E+00
1.84E+00
2.30E+00
2.70E+00
3.53E+00
4.27E+00
5.90E+00
7.24E+00
9.61E+00
1.16E+01
1.34E+01
1.50E+01
1.80E+01
2.08E+01
2.67E+01
3.21E+01
4.07E+01
4.73E+01
5.26E+01
5.86E+01
6.42E+01
6.89E+01
7.64E+01
8.10E+01
8.77E+01
9.23E+01
9.40E+01
9.58E+01
9.83E+01
1.01E+02

1.16E-02
1.53E-02
1.99E-02
2.60E-02
3.39E-02
4.29E-02
6.24E-02
7.27E-02
9.36E-02
1.16E-01
1.48E-01
1.93E-01
2.19E-01
2.54E-01
2.74E-01
2.91E-01
3.11E-01
3.41E-01
4.10E-01
6.07E-01
8.26E-01
1.27E+00
1.72E+00
2.17E+00
2.58E+00
3.37E+00
4.11E+00
5.70E+00
6.96E+00
9.36E+00
1.14E+01
1.34E+01
1.49E+01
1.80E+01
2.09E+01
2.75E+01
3.32E+01
4.34E+01
5.17E+01
5.84E+01
6.53E+01
7.35E+01
7.91E+01
8.88E+01
9.58E+01
1.04E+02
1.10E+02
1.13E+02
1.15E+02
1.19E+02
1.22E+02

9.41E-03
1.20E-02
1.51E-02
1.93E-02
2.46E-02
3.09E-02
4.50E-02
5.19E-02
6.56E-02
7.98E-02
1.01E-01
1.38E-01
1.62E-01
1.97E-01
2.12E-01
2.31E-01
2.52E-01
2.78E-01
3.32E-01
5.04E-01
7.00E-01
1.10E+00
1.50E+00
1.90E+00
2.26E+00
2.96E+00
3.62E+00
5.26E+00
6.55E+00
8.75E+00
1.06E+01
1.25E+01
1.42E+01
1.73E+01
2.05E+01
2.73E+01
3.41E+01
4.56E+01
5.64E+01
6.53E+01
7.44E+01
8.55E+01
9.32E+01
1.06E+02
1.15E+02
1.26E+02
1.34E+02
1.38E+02
1.43E+02
1.48E+02
1.52E+02

6.87E-03
8.29E-03
9.92E-03
1.21E-02
1.49E-02
1.89E-02
2.71E-02
3.15E-02
4.16E-02
4.97E-02
6.54E-02
8.55E-02
1.09E-01
1.38E-01
1.58E-01
1.74E-01
1.91E-01
2.11E-01
2.55E-01
3.91E-01
5.46E-01
8.80E-01
1.23E+00
1.57E+00
1.91E+00
2.57E+00
3.21E+00
4.66E+00
5.94E+00
8.18E+00
1.02E+01
1.20E+01
1.37E+01
1.69E+01
2.00E+01
2.73E+01
3.44E+01
4.80E+01
6.09E+01
7.23E+01
8.21E+01
9.81E+01
1.10E+02
1.30E+02
1.44E+02
1.61E+02
1.73E+02
1.81E+02
1.87E+02
1.95E+02
2.02E+02

180

ROT

ISO

SS-ISO

IS-ISO

1.33E-02
1.59E-02
1.78E-02
1.87E-02
1.86E-02
1.84E-02
1.62E-02
1.56E-02
1.55E-02
1.75E-02
2.61E-02
5.64E-02
9.46E-02
1.63E-01
2.09E-01
2.43E-01
2.73E-01
3.02E-01
3.63E-01
5.43E-01
7.45E-01
1.16E+00
1.58E+00
1.99E+00
2.39E+00
3.14E+00
3.84E+00
5.41E+00
6.77E+00
9.13E+00
1.12E+01
1.32E+01
1.50E+01
1.86E+01
2.21E+01
3.04E+01
3.82E+01
5.13E+01
6.18E+01
7.01E+01
7.65E+01
8.62E+01
9.27E+01
1.03E+02
1.10E+02
1.18E+02
1.23E+02
1.27E+02
1.30E+02
1.34E+02
1.37E+02

1.15E-02
1.41E-02
1.74E-02
2.16E-02
2.73E-02
3.37E-02
4.70E-02
5.32E-02
6.65E-02
7.83E-02
9.88E-02
1.30E-01
1.59E-01
1.99E-01
2.26E-01
2.48E-01
2.73E-01
2.97E-01
3.56E-01
5.29E-01
7.22E-01
1.12E+00
1.53E+00
1.92E+00
2.31E+00
3.04E+00
3.73E+00
5.24E+00
6.56E+00
8.85E+00
1.09E+01
1.27E+01
1.44E+01
1.76E+01
2.07E+01
2.77E+01
3.44E+01
4.60E+01
5.60E+01
6.43E+01
7.11E+01
8.18E+01
8.95E+01
1.02E+02
1.10E+02
1.21E+02
1.28E+02
1.32E+02
1.36E+02
1.41E+02
1.45E+02

1.04E-02
1.28E-02
1.58E-02
1.94E-02
2.36E-02
2.88E-02
3.95E-02
4.49E-02
5.60E-02
6.50E-02
8.13E-02
1.04E-01
1.27E-01
1.58E-01
1.80E-01
1.98E-01
2.18E-01
2.38E-01
2.86E-01
4.29E-01
5.89E-01
9.32E-01
1.28E+00
1.63E+00
1.97E+00
2.62E+00
3.25E+00
4.67E+00
5.91E+00
8.08E+00
1.00E+01
1.18E+01
1.35E+01
1.66E+01
1.97E+01
2.68E+01
3.38E+01
4.61E+01
5.69E+01
6.61E+01
7.41E+01
8.71E+01
9.75E+01
1.16E+02
1.29E+02
1.47E+02
1.59E+02
1.67E+02
1.74E+02
1.85E+02
1.93E+02

1.05E-02
1.31E-02
1.61E-02
2.00E-02
2.45E-02
3.01E-02
4.06E-02
4.58E-02
5.77E-02
6.54E-02
8.22E-02
1.05E-01
1.29E-01
1.62E-01
1.84E-01
2.04E-01
2.23E-01
2.46E-01
2.95E-01
4.45E-01
6.10E-01
9.64E-01
1.32E+00
1.67E+00
2.02E+00
2.70E+00
3.32E+00
4.74E+00
6.03E+00
8.22E+00
1.02E+01
1.20E+01
1.37E+01
1.69E+01
1.99E+01
2.68E+01
3.39E+01
4.61E+01
5.66E+01
6.58E+01
7.35E+01
8.55E+01
9.61E+01
1.15E+02
1.25E+02
1.40E+02
1.50E+02
1.58E+02
1.65E+02
1.74E+02
1.80E+02

1.02E-02
1.25E-02
1.53E-02
1.87E-02
2.26E-02
2.75E-02
3.75E-02
4.26E-02
5.43E-02
6.32E-02
8.02E-02
1.01E-01
1.25E-01
1.54E-01
1.76E-01
1.94E-01
2.09E-01
2.32E-01
2.79E-01
4.13E-01
5.68E-01
9.00E-01
1.24E+00
1.59E+00
1.92E+00
2.54E+00
3.18E+00
4.58E+00
5.77E+00
7.94E+00
9.80E+00
1.16E+01
1.33E+01
1.63E+01
1.93E+01
2.62E+01
3.37E+01
4.61E+01
5.72E+01
6.66E+01
7.47E+01
8.89E+01
9.89E+01
1.18E+02
1.35E+02
1.54E+02
1.68E+02
1.78E+02
1.83E+02
1.96E+02
2.06E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

421
422
423
424
425
426
427
428
429
430
431
432
433
434
435

Figure A.2.1a Conversion coefficients from photon fluence to personal dose (ICRP, 2010; Endo, 2016b,
2017).

FINAL DRAFT JULY 2017

436
437

NOT TO BE REFERENCED

Table A.2.1b Conversion coefficients from photon air kerma to personal dose (ICRP, 2010; Endo,
2016b, 2017).
hp() / (Sv Gy-1)
Ep / MeV
5.0E-03
6.0E-03
7.0E-038.0E-03
9.0E-03
1.0E-02
1.2E-02
1.3E-02
1.5E-02
1.7E-022.0E-02
2.5E-02
3.0E-02
4.0E-02
5.0E-02
6.0E-02
7.0E-028.0E-02
1.0E-01
1.5E-01
2.0E-01
3.0E-01
4.0E-01
5.0E-01
6.0E-01
8.0E-01
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01

438
439

0
4.36E-04
7.80E-04
1.45E-03
2.84E-03
5.31E-03
9.26E-03
2.09E-02
2.87E-02
4.99E-02
7.56E-02
1.34E-01
2.60E-01
4.32E-01
8.16E-01
1.14E+00
1.35E+00
1.43E+00
1.44E+00
1.39E+00
1.25E+00
1.17E+00
1.09E+00
1.06E+00
1.04E+00
1.02E+00
1.01E+00
1.00E+00
9.96E-01
9.90E-01
9.77E-01
9.64E-01
9.45E-01
9.28E-01
8.84E-01
8.50E-01
7.57E-01
6.79E-01
5.53E-01
4.63E-01
3.95E-01

max(15) max(30) max(45) max(60) max(75) max(90)
4.61E-04
8.47E-04
1.58E-03
2.98E-03
5.44E-03
9.15E-03
2.08E-02
2.86E-02
4.87E-02
7.54E-02
1.30E-01
2.56E-01
4.25E-01
8.00E-01
1.12E+00
1.33E+00
1.43E+00
1.43E+00
1.39E+00
1.26E+00
1.17E+00
1.10E+00
1.06E+00
1.04E+00
1.03E+00
1.01E+00
1.02E+00
1.00E+00
9.97E-01
9.86E-01
9.67E-01
9.44E-01
9.32E-01
8.94E-01
8.54E-01
7.68E-01
6.84E-01
5.60E-01
4.67E-01
3.98E-01

4.55E-04
8.55E-04
1.58E-03
2.90E-03
5.10E-03
8.41E-03
1.90E-02
2.62E-02
4.49E-02
7.04E-02
1.22E-01
2.43E-01
4.06E-01
7.71E-01
1.09E+00
1.27E+00
1.36E+00
1.37E+00
1.32E+00
1.20E+00
1.13E+00
1.05E+00
1.03E+00
1.01E+00
1.00E+00
9.89E-01
9.87E-01
9.86E-01
9.81E-01
9.68E-01
9.59E-01
9.40E-01
9.23E-01
8.99E-01
8.61E-01
7.70E-01
6.93E-01
5.64E-01
4.81E-01
4.11E-01

4.26E-04
8.12E-04
1.47E-03
2.60E-03
4.44E-03
7.17E-03
1.59E-02
2.21E-02
3.82E-02
6.04E-02
1.07E-01
2.19E-01
3.62E-01
6.91E-01
9.72E-01
1.14E+00
1.23E+00
1.24E+00
1.23E+00
1.11E+00
1.05E+00
9.98E-01
9.74E-01
9.65E-01
9.50E-01
9.54E-01
9.52E-01
9.60E-01
9.59E-01
9.63E-01
9.56E-01
9.45E-01
9.25E-01
8.95E-01
8.61E-01
7.75E-01
7.08E-01
5.93E-01
5.07E-01
4.41E-01

3.79E-04
7.18E-04
1.29E-03
2.21E-03
3.67E-03
5.80E-03
1.24E-02
1.72E-02
3.00E-02
4.84E-02
8.76E-02
1.83E-01
3.04E-01
5.92E-01
8.50E-01
1.01E+00
1.08E+00
1.11E+00
1.11E+00
1.01E+00
9.64E-01
9.20E-01
9.08E-01
9.13E-01
9.08E-01
9.09E-01
9.17E-01
9.28E-01
9.21E-01
9.38E-01
9.38E-01
9.42E-01
9.21E-01
8.96E-01
8.68E-01
7.97E-01
7.31E-01
6.32E-01
5.54E-01
4.90E-01

3.07E-04
5.64E-04
9.77E-04
1.64E-03
2.67E-03
4.18E-03
8.96E-03
1.22E-02
2.10E-02
3.34E-02
6.02E-02
1.31E-01
2.25E-01
4.59E-01
6.57E-01
8.01E-01
8.74E-01
9.05E-01
8.94E-01
8.41E-01
8.17E-01
7.96E-01
7.91E-01
7.97E-01
7.93E-01
7.99E-01
8.09E-01
8.55E-01
8.67E-01
8.77E-01
8.76E-01
8.81E-01
8.77E-01
8.61E-01
8.50E-01
7.94E-01
7.51E-01
6.65E-01
6.05E-01
5.48E-01

2.24E-04
3.90E-04
6.40E-04
1.02E-03
1.62E-03
2.55E-03
5.39E-03
7.43E-03
1.33E-02
2.08E-02
3.88E-02
8.10E-02
1.51E-01
3.22E-01
4.89E-01
6.02E-01
6.64E-01
6.88E-01
6.87E-01
6.52E-01
6.37E-01
6.36E-01
6.50E-01
6.60E-01
6.72E-01
6.94E-01
7.16E-01
7.58E-01
7.86E-01
8.20E-01
8.40E-01
8.46E-01
8.47E-01
8.40E-01
8.29E-01
7.92E-01
7.58E-01
7.00E-01
6.53E-01
6.07E-01

180

ROT

ISO

SS-ISO

IS-ISO

4.35E-04
7.47E-04
1.15E-03
1.59E-03
2.02E-03
2.49E-03
3.23E-03
3.67E-03
4.96E-03
7.31E-03
1.55E-02
5.34E-02
1.31E-01
3.80E-01
6.47E-01
8.41E-01
9.49E-01
9.85E-01
9.77E-01
9.06E-01
8.70E-01
8.39E-01
8.35E-01
8.36E-01
8.40E-01
8.48E-01
8.57E-01
8.80E-01
8.96E-01
9.15E-01
9.23E-01
9.31E-01
9.28E-01
9.24E-01
9.16E-01
8.82E-01
8.42E-01
7.48E-01
6.62E-01
5.88E-01

3.74E-04
6.62E-04
1.12E-03
1.84E-03
2.96E-03
4.55E-03
9.36E-03
1.26E-02
2.13E-02
3.28E-02
5.87E-02
1.23E-01
2.20E-01
4.64E-01
7.00E-01
8.58E-01
9.49E-01
9.68E-01
9.59E-01
8.83E-01
8.43E-01
8.10E-01
8.09E-01
8.07E-01
8.12E-01
8.21E-01
8.32E-01
8.52E-01
8.68E-01
8.87E-01
8.98E-01
8.96E-01
8.91E-01
8.74E-01
8.58E-01
8.04E-01
7.58E-01
6.71E-01
6.00E-01
5.39E-01

3.39E-04
6.05E-04
1.02E-03
1.64E-03
2.56E-03
3.89E-03
7.87E-03
1.06E-02
1.79E-02
2.72E-02
4.83E-02
9.81E-02
1.76E-01
3.68E-01
5.57E-01
6.85E-01
7.57E-01
7.76E-01
7.70E-01
7.16E-01
6.88E-01
6.74E-01
6.77E-01
6.85E-01
6.93E-01
7.08E-01
7.25E-01
7.60E-01
7.82E-01
8.10E-01
8.24E-01
8.32E-01
8.35E-01
8.25E-01
8.16E-01
7.78E-01
7.45E-01
6.72E-01
6.10E-01
5.55E-01

3.42E-04
6.15E-04
1.04E-03
1.69E-03
2.66E-03
4.07E-03
8.09E-03
1.08E-02
1.85E-02
2.74E-02
4.88E-02
9.92E-02
1.79E-01
3.78E-01
5.70E-01
7.06E-01
7.74E-01
8.02E-01
7.94E-01
7.42E-01
7.12E-01
6.97E-01
6.98E-01
7.02E-01
7.10E-01
7.29E-01
7.41E-01
7.71E-01
7.98E-01
8.24E-01
8.40E-01
8.46E-01
8.47E-01
8.40E-01
8.25E-01
7.77E-01
7.47E-01
6.72E-01
6.07E-01
5.52E-01

3.33E-04
5.90E-04
9.89E-04
1.58E-03
2.45E-03
3.72E-03
7.47E-03
1.01E-02
1.74E-02
2.64E-02
4.76E-02
9.57E-02
1.73E-01
3.59E-01
5.45E-01
6.72E-01
7.27E-01
7.56E-01
7.51E-01
6.89E-01
6.63E-01
6.51E-01
6.55E-01
6.68E-01
6.75E-01
6.86E-01
7.10E-01
7.46E-01
7.64E-01
7.96E-01
8.07E-01
8.18E-01
8.23E-01
8.10E-01
8.00E-01
7.59E-01
7.43E-01
6.72E-01
6.13E-01
5.59E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

440
441
442
443
444
445
446
447
448
449
450
451
452
453
454
455
456
457

Figure A.2.1b Conversion coefficients from photon air kerma to personal dose (ICRP, 2010;
Endo, 2016b, 2017).

FINAL DRAFT JULY 2017458

NOT TO BE REFERENCED

Table A.2.2 Conversion coefficients from neutron fluence to personal dose (ICRP, 2010; Endo, 2017).
hp() / (pSv cm2)
Ep / MeV
1.0E-09
1.0E-08
2.5E-08
1.0E-072.0E-07
5.0E-07
1.0E-06
2.0E-06
5.0E-06
1.0E-05
2.0E-05
5.0E-05
1.0E-04
2.0E-04
5.0E-04
1.0E-032.0E-035.0E-03
1.0E-022.0E-02
3.0E-02
5.0E-02
7.0E-02
1.0E-01
1.5E-01
2.0E-01
3.0E-01
5.0E-01
7.0E-01
9.0E-01
1.0E+00
1.2E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
7.0E+00
8.0E+00
9.0E+00
1.0E+01
1.2E+01
1.4E+01
1.5E+01
1.6E+01
1.8E+01
2.0E+01
2.1E+01
3.0E+01
5.0E+01
7.5E+01
1.0E+02
1.3E+02
1.5E+02
1.8E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
7.0E+02
8.0E+02
9.0E+02
1.0E+030
3.09E+00
3.55E+00
4.00E+00
5.20E+00
5.87E+00
6.59E+00
7.03E+00
7.39E+00
7.71E+00
7.82E+00
7.84E+00
7.82E+00
7.79E+00
7.73E+00
7.54E+00
7.54E+00
7.61E+00
7.97E+00
9.11E+00
1.22E+01
1.57E+01
2.30E+01
3.06E+01
4.19E+01
6.06E+01
7.88E+01
1.14E+02
1.77E+02
2.32E+02
2.79E+02
3.01E+02
3.30E+02
3.65E+02
4.07E+02
4.58E+02
4.83E+02
4.94E+02
4.98E+02
4.99E+02
4.99E+02
5.00E+02
5.00E+02
4.99E+02
4.95E+02
4.93E+02
4.90E+02
4.84E+02
4.77E+02
4.74E+02
4.53E+02
4.33E+02
4.20E+02
4.02E+02
3.82E+02
3.73E+02
3.63E+02
3.59E+02
3.63E+02
3.89E+02
4.22E+02
4.57E+02
4.86E+02
5.08E+02
5.24E+02
5.37E+02

max(15) max(30) max(45) max(60) max(75) max(90)
2.95E+00
3.52E+00
3.96E+00
5.11E+00
5.83E+00
6.67E+00
7.03E+00
7.46E+00
7.80E+00
7.89E+00
7.93E+00
7.88E+00
7.82E+00
7.83E+00
7.68E+00
7.59E+00
7.69E+00
8.15E+00
9.26E+00
1.24E+01
1.61E+01
2.34E+01
3.12E+01
4.25E+01
6.11E+01
7.96E+01
1.14E+02
1.80E+02
2.35E+02
2.83E+02
2.89E+02
3.34E+02
3.71E+02
4.12E+02
4.58E+02
4.91E+02
4.93E+02
5.00E+02
4.97E+02
4.94E+02
4.95E+02
5.07E+02
5.10E+02
4.98E+02
4.95E+02
4.89E+02
4.67E+02
4.65E+02
4.10E+02
4.29E+02
4.01E+02
4.12E+02
4.14E+02
4.24E+02
4.20E+02
4.08E+02
4.08E+02
3.84E+02
4.03E+02
4.39E+02
4.76E+02
4.97E+02
5.12E+02
5.25E+02
5.35E+02

2.70E+00
3.23E+00
3.55E+00
4.71E+00
5.27E+00
6.16E+00
6.51E+00
6.83E+00
7.11E+00
7.24E+00
7.26E+00
7.21E+00
7.22E+00
7.15E+00
7.12E+00
7.06E+00
7.08E+00
7.51E+00
8.61E+00
1.15E+01
1.48E+01
2.18E+01
2.91E+01
3.94E+01
5.71E+01
7.43E+01
1.07E+02
1.70E+02
2.23E+02
2.70E+02
2.76E+02
3.18E+02
3.56E+02
3.96E+02
4.42E+02
4.78E+02
4.79E+02
4.86E+02
4.83E+02
4.83E+02
4.82E+02
4.92E+02
4.96E+02
4.89E+02
4.86E+02
4.80E+02
4.65E+02
4.62E+02
4.04E+02
4.24E+02
4.00E+02
4.14E+02
4.19E+02
4.32E+02
4.25E+02
4.12E+02
4.13E+02
3.92E+02
4.13E+02
4.54E+02
4.88E+02
5.10E+02
5.27E+02
5.40E+02
5.45E+02

2.34E+00
2.77E+00
3.07E+00
4.08E+00
4.62E+00
5.34E+00
5.70E+00
5.90E+00
6.13E+00
6.24E+00
6.28E+00
6.32E+00
6.18E+00
6.26E+00
6.15E+00
6.10E+00
6.21E+00
6.44E+00
7.45E+00
9.95E+00
1.29E+01
1.87E+01
2.50E+01
3.45E+01
5.00E+01
6.55E+01
9.45E+01
1.52E+02
2.00E+02
2.41E+02
2.48E+02
2.90E+02
3.25E+02
3.65E+02
4.14E+02
4.46E+02
4.59E+02
4.66E+02
4.63E+02
4.60E+02
4.65E+02
4.76E+02
4.77E+02
4.72E+02
4.70E+02
4.67E+02
4.46E+02
4.47E+02
3.98E+02
4.19E+02
4.01E+02
4.10E+02
4.21E+02
4.41E+02
4.41E+02
4.35E+02
4.35E+02
4.08E+02
4.28E+02
4.70E+02
5.09E+02
5.26E+02
5.48E+02
5.59E+02
5.70E+02

1.94E+00
2.30E+00
2.52E+00
3.32E+00
3.76E+00
4.34E+00
4.57E+00
4.82E+00
5.06E+00
5.13E+00
5.07E+00
5.12E+00
5.18E+00
5.11E+00
5.03E+00
4.99E+00
4.97E+00
5.28E+00
6.10E+00
8.16E+00
1.04E+01
1.54E+01
2.03E+01
2.83E+01
4.10E+01
5.37E+01
7.85E+01
1.26E+02
1.69E+02
2.03E+02
2.08E+02
2.45E+02
2.79E+02
3.19E+02
3.70E+02
3.99E+02
4.19E+02
4.27E+02
4.29E+02
4.29E+02
4.30E+02
4.39E+02
4.46E+02
4.42E+02
4.42E+02
4.38E+02
4.24E+02
4.26E+02
3.89E+02
4.05E+02
3.94E+02
4.09E+02
4.26E+02
4.49E+02
4.47E+02
4.52E+02
4.58E+02
4.35E+02
4.47E+02
4.92E+02
5.31E+02
5.51E+02
5.74E+02
5.83E+02
5.94E+02

1.45E+00
1.68E+00
1.91E+00
2.51E+00
2.79E+00
3.28E+00
3.49E+00
3.69E+00
3.74E+00
3.89E+00
3.89E+00
3.85E+00
3.85E+00
3.86E+00
3.82E+00
3.76E+00
3.76E+00
4.03E+00
4.55E+00
6.11E+00
7.93E+00
1.15E+01
1.54E+01
2.10E+01
3.08E+01
4.03E+01
5.89E+01
9.47E+01
1.28E+02
1.56E+02
1.57E+02
1.90E+02
2.20E+02
2.57E+02
3.08E+02
3.32E+02
3.57E+02
3.69E+02
3.81E+02
3.78E+02
3.86E+02
3.93E+02
3.96E+02
4.00E+02
3.99E+02
4.00E+02
3.88E+02
3.91E+02
3.62E+02
3.91E+02
3.87E+02
4.05E+02
4.26E+02
4.50E+02
4.58E+02
4.59E+02
4.72E+02
4.53E+02
4.68E+02
5.15E+02
5.54E+02
5.76E+02
6.00E+02
6.09E+02
6.22E+02

1.04E+00
1.15E+00
1.32E+00
1.70E+00
1.94E+00
2.21E+00
2.40E+00
2.52E+00
2.64E+00
2.65E+00
2.68E+00
2.66E+00
2.65E+00
2.66E+00
2.62E+00
2.61E+00
2.60E+00
2.74E+00
3.13E+00
4.21E+00
5.40E+00
7.91E+00
1.05E+01
1.44E+01
2.08E+01
2.72E+01
3.97E+01
6.37E+01
8.55E+01
1.05E+02
1.15E+02
1.30E+02
1.50E+02
1.79E+02
2.21E+02
2.49E+02
2.69E+02
2.84E+02
2.95E+02
3.03E+02
3.10E+02
3.16E+02
3.25E+02
3.33E+02
3.36E+02
3.38E+02
3.43E+02
3.47E+02
3.48E+02
3.60E+02
3.80E+02
3.99E+02
4.09E+02
4.16E+02
4.20E+02
4.25E+02
4.29E+02
4.51E+02
4.83E+02
5.23E+02
5.63E+02
5.97E+02
6.20E+02
6.38E+02
6.51E+02

180

ROT

ISO

SS-ISO

IS-ISO

1.85E+00
2.11E+00
2.44E+00
3.25E+00
3.72E+00
4.33E+00
4.73E+00
5.02E+00
5.30E+00
5.44E+00
5.51E+00
5.55E+00
5.57E+00
5.59E+00
5.60E+00
5.60E+00
5.62E+00
5.95E+00
6.81E+00
8.93E+00
1.12E+01
1.57E+01
2.00E+01
2.59E+01
3.49E+01
4.31E+01
5.81E+01
8.59E+01
1.12E+02
1.36E+02
1.48E+02
1.67E+02
1.95E+02
2.35E+02
2.92E+02
3.30E+02
3.54E+02
3.71E+02
3.83E+02
3.92E+02
3.98E+02
4.04E+02
4.12E+02
4.17E+02
4.19E+02
4.20E+02
4.22E+02
4.23E+02
4.23E+02
4.22E+02
4.28E+02
4.39E+02
4.44E+02
4.46E+02
4.46E+02
4.47E+02
4.48E+02
4.64E+02
4.96E+02
5.33E+02
5.69E+02
5.99E+02
6.23E+02
6.40E+02
6.54E+02

1.70E+00
2.03E+00
2.31E+00
2.98E+00
3.36E+00
3.86E+00
4.17E+00
4.40E+00
4.59E+00
4.68E+00
4.72E+00
4.73E+00
4.72E+00
4.67E+00
4.60E+00
4.58E+00
4.61E+00
4.86E+00
5.57E+00
7.41E+00
9.46E+00
1.37E+01
1.80E+01
2.43E+01
3.47E+01
4.47E+01
6.38E+01
9.91E+01
1.31E+02
1.60E+02
1.74E+02
1.93E+02
2.19E+02
2.54E+02
3.01E+02
3.31E+02
3.51E+02
3.65E+02
3.74E+02
3.81E+02
3.86E+02
3.90E+02
3.95E+02
3.98E+02
3.98E+02
3.99E+02
3.99E+02
3.98E+02
3.98E+02
3.95E+02
3.95E+02
4.02E+02
4.06E+02
4.11E+02
4.14E+02
4.18E+02
4.22E+02
4.43E+02
4.72E+02
5.03E+02
5.32E+02
5.58E+02
5.80E+02
5.98E+02
6.14E+02

1.29E+00
1.56E+00
1.76E+00
2.26E+00
2.54E+00
2.92E+00
3.15E+00
3.32E+00
3.47E+00
3.52E+00
3.54E+00
3.55E+00
3.54E+00
3.52E+00
3.47E+00
3.46E+00
3.48E+00
3.66E+00
4.19E+00
5.61E+00
7.18E+00
1.04E+01
1.37E+01
1.86E+01
2.66E+01
3.44E+01
4.94E+01
7.71E+01
1.02E+02
1.26E+02
1.37E+02
1.53E+02
1.74E+02
2.03E+02
2.44E+02
2.71E+02
2.90E+02
3.03E+02
3.13E+02
3.21E+02
3.27E+02
3.32E+02
3.39E+02
3.44E+02
3.46E+02
3.47E+02
3.50E+02
3.52E+02
3.53E+02
3.58E+02
3.71E+02
3.87E+02
3.97E+02
4.07E+02
4.12E+02
4.21E+02
4.26E+02
4.55E+02
4.88E+02
5.21E+02
5.53E+02
5.80E+02
6.04E+02
6.24E+02
6.42E+02

1.35E+00
1.58E+00
1.76E+00
2.33E+00
2.61E+00
2.99E+00
3.25E+00
3.37E+00
3.56E+00
3.62E+00
3.60E+00
3.65E+00
3.64E+00
3.64E+00
3.67E+00
3.64E+00
3.64E+00
3.88E+00
4.38E+00
5.80E+00
7.66E+00
1.10E+01
1.47E+01
1.94E+01
2.77E+01
3.57E+01
5.11E+01
7.97E+01
1.08E+02
1.30E+02
1.31E+02
1.57E+02
1.83E+02
2.13E+02
2.58E+02
2.81E+02
3.05E+02
3.15E+02
3.28E+02
3.29E+02
3.32E+02
3.40E+02
3.49E+02
3.56E+02
3.59E+02
3.62E+02
3.65E+02
3.73E+02
3.35E+02
3.66E+02
3.46E+02
3.53E+02
3.73E+02
4.12E+02
4.09E+02
4.22E+02
4.33E+02
4.37E+02
4.61E+02
5.09E+02
5.66E+02
6.25E+02
6.38E+02
6.45E+02
6.63E+02

1.23E+00
1.54E+00
1.76E+00
2.19E+00
2.47E+00
2.85E+00
3.05E+00
3.27E+00
3.38E+00
3.42E+00
3.48E+00
3.45E+00
3.44E+00
3.40E+00
3.27E+00
3.28E+00
3.32E+00
3.44E+00
4.00E+00
5.42E+00
6.70E+00
9.80E+00
1.27E+01
1.78E+01
2.55E+01
3.31E+01
4.77E+01
7.45E+01
9.60E+01
1.22E+02
1.43E+02
1.49E+02
1.65E+02
1.93E+02
2.30E+02
2.61E+02
2.75E+02
2.91E+02
2.98E+02
3.13E+02
3.22E+02
3.24E+02
3.29E+02
3.32E+02
3.33E+02
3.32E+02
3.35E+02
3.31E+02
3.71E+02
3.50E+02
3.96E+02
4.21E+02
4.21E+02
4.02E+02
4.15E+02
4.20E+02
4.19E+02
4.73E+02
5.15E+02
5.33E+02
5.40E+02
5.35E+02
5.70E+02
6.03E+02
6.21E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

459
460
461
462
463
464
465
466
467
468
469
470
471
472
473
474
475

Figure A.2.2 Conversion coefficients from neutron fluence to personal dose (ICRP, 2010; Endo,2017).

FINAL DRAFT JULY 2017476

NOT TO BE REFERENCED

Table A.2.3 Conversion coefficients from electron fluence to personal dose (ICRP, 2010; Endo, 2017).
hp() / (pSv cm2)
Ep / MeV
1.0E-02
1.5E-022.0E-02
3.0E-02
4.0E-02
5.0E-02
6.0E-028.0E-02
1.0E-01
1.5E-01
2.0E-01
3.0E-01
4.0E-01
5.0E-01
6.0E-01
8.0E-01
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01
6.0E+01
8.0E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
8.0E+02
1.0E+03

477
478

0
2.69E-02
4.04E-02
5.39E-02
8.10E-02
1.08E-01
1.35E-01
1.63E-01
2.18E-01
2.75E-01
4.18E-01
5.69E-01
8.89E-01
1.24E+00
1.63E+00
2.05E+00
4.04E+00
7.10E+00
1.50E+01
2.24E+01
3.61E+01
4.82E+01
5.93E+01
7.06E+01
9.79E+01
1.25E+02
1.88E+02
2.36E+02
3.02E+02
3.29E+02
3.37E+02
3.41E+02
3.46E+02
3.49E+02
3.55E+02
3.59E+02
3.65E+02
3.69E+02
3.72E+02
3.75E+02
3.79E+02
3.82E+02

max(15) max(30) max(45) max(60) max(75) max(90)
2.60E-02
3.89E-02
5.17E-02
7.76E-02
1.04E-01
1.30E-01
1.56E-01
2.10E-01
2.64E-01
4.03E-01
5.49E-01
8.68E-01
1.22E+00
1.61E+00
2.07E+00
3.82E+00
6.62E+00
1.41E+01
2.14E+01
3.47E+01
4.73E+01
5.90E+01
7.02E+01
9.72E+01
1.27E+02
1.88E+02
2.36E+02
3.05E+02
3.34E+02
3.41E+02
3.46E+02
3.51E+02
3.52E+02
3.58E+02
3.61E+02
3.68E+02
3.70E+02
3.74E+02
3.78E+02
3.79E+02
3.83E+02

2.44E-02
3.65E-02
4.86E-02
7.29E-02
9.77E-02
1.22E-01
1.47E-01
1.98E-01
2.50E-01
3.86E-01
5.30E-01
8.55E-01
1.23E+00
1.66E+00
2.16E+00
3.75E+00
6.16E+00
1.28E+01
1.94E+01
3.17E+01
4.35E+01
5.50E+01
6.63E+01
9.40E+01
1.23E+02
1.82E+02
2.27E+02
2.91E+02
3.26E+02
3.39E+02
3.43E+02
3.50E+02
3.54E+02
3.60E+02
3.64E+02
3.69E+02
3.74E+02
3.76E+02
3.79E+02
3.86E+02
3.88E+02

2.21E-02
3.29E-02
4.38E-02
6.58E-02
8.81E-02
1.10E-01
1.33E-01
1.79E-01
2.26E-01
3.51E-01
4.86E-01
7.96E-01
1.16E+00
1.58E+00
2.06E+00
3.41E+00
5.33E+00
1.07E+01
1.62E+01
2.66E+01
3.68E+01
4.70E+01
5.69E+01
8.37E+01
1.14E+02
1.70E+02
2.11E+02
2.75E+02
3.11E+02
3.34E+02
3.41E+02
3.51E+02
3.55E+02
3.66E+02
3.67E+02
3.76E+02
3.83E+02
3.86E+02
3.91E+02
3.96E+02
4.02E+02

1.98E-02
2.95E-02
3.92E-02
5.89E-02
7.89E-02
9.88E-02
1.19E-01
1.60E-01
2.02E-01
3.13E-01
4.34E-01
7.04E-01
1.02E+00
1.38E+00
1.79E+00
2.86E+00
4.24E+00
8.19E+00
1.24E+01
2.06E+01
2.86E+01
3.68E+01
4.54E+01
6.74E+01
9.21E+01
1.43E+02
1.85E+02
2.45E+02
2.90E+02
3.18E+02
3.33E+02
3.51E+02
3.57E+02
3.72E+02
3.78E+02
3.90E+02
3.97E+02
4.04E+02
4.10E+02
4.14E+02
4.25E+02

1.67E-02
2.50E-02
3.32E-02
4.99E-02
6.68E-02
8.37E-02
1.01E-01
1.35E-01
1.70E-01
2.61E-01
3.59E-01
5.66E-01
8.00E-01
1.07E+00
1.35E+00
2.06E+00
2.96E+00
5.58E+00
8.41E+00
1.42E+01
2.01E+01
2.58E+01
3.24E+01
4.68E+01
6.55E+01
1.08E+02
1.42E+02
2.02E+02
2.56E+02
2.97E+02
3.22E+02
3.47E+02
3.58E+02
3.76E+02
3.87E+02
4.05E+02
4.17E+02
4.24E+02
4.31E+02
4.43E+02
4.51E+02

1.35E-02
2.02E-02
2.70E-02
4.05E-02
5.41E-02
6.77E-02
8.13E-02
1.09E-01
1.36E-01
2.06E-01
2.78E-01
4.27E-01
5.83E-01
7.50E-01
9.23E-01
1.33E+00
1.82E+00
3.22E+00
4.87E+00
8.62E+00
1.26E+01
1.66E+01
2.09E+01
3.08E+01
4.26E+01
7.02E+01
9.47E+01
1.38E+02
1.89E+02
2.44E+02
2.79E+02
3.21E+02
3.43E+02
3.72E+02
3.93E+02
4.24E+02
4.42E+02
4.55E+02
4.66E+02
4.89E+02
5.04E+02

180

ROT

ISO

SS-ISO

IS-ISO

2.68E-02
4.02E-02
5.35E-02
8.01E-02
1.07E-01
1.33E-01
1.60E-01
2.13E-01
2.67E-01
3.99E-01
5.30E-01
7.87E-01
1.04E+00
1.28E+00
1.50E+00
1.68E+00
1.68E+00
1.62E+00
1.62E+00
1.95E+00
2.62E+00
3.63E+00
5.04E+00
9.46E+00
1.83E+01
5.31E+01
1.04E+02
2.20E+02
2.97E+02
3.31E+02
3.44E+02
3.58E+02
3.66E+02
3.79E+02
3.88E+02
3.99E+02
4.08E+02
4.14E+02
4.19E+02
4.28E+02
4.34E+02

2.13E-02
3.17E-02
4.22E-02
6.34E-02
8.48E-02
1.06E-01
1.27E-01
1.70E-01
2.13E-01
3.23E-01
4.37E-01
6.73E-01
9.21E-01
1.19E+00
1.48E+00
2.23E+00
3.23E+00
5.93E+00
8.73E+00
1.42E+01
1.96E+01
2.50E+01
3.07E+01
4.43E+01
5.87E+01
9.63E+01
1.34E+02
2.03E+02
2.56E+02
2.90E+02
3.12E+02
3.37E+02
3.51E+02
3.70E+02
3.84E+02
3.98E+02
4.08E+02
4.16E+02
4.24E+02
4.37E+02
4.47E+02

1.88E-02
2.83E-02
3.77E-02
5.67E-02
7.58E-02
9.48E-02
1.14E-01
1.52E-01
1.91E-01
2.91E-01
3.93E-01
6.06E-01
8.32E-01
1.08E+00
1.35E+00
1.97E+00
2.76E+00
4.96E+00
7.24E+00
1.19E+01
1.64E+01
2.10E+01
2.55E+01
3.55E+01
4.67E+01
7.69E+01
1.06E+02
1.64E+02
2.12E+02
2.49E+02
2.75E+02
3.09E+02
3.31E+02
3.63E+02
3.83E+02
4.10E+02
4.30E+02
4.45E+02
4.57E+02
4.78E+02
4.95E+02

1.89E-02
2.84E-02
3.78E-02
5.70E-02
7.59E-02
9.50E-02
1.15E-01
1.54E-01
1.92E-01
2.94E-01
3.96E-01
6.16E-01
8.51E-01
1.09E+00
1.38E+00
2.03E+00
2.86E+00

1.87E-02
2.82E-02
3.76E-02
5.64E-02
7.57E-02
9.46E-02
1.13E-01
1.50E-01
1.90E-01
2.88E-01
3.90E-01
5.96E-01
8.13E-01
1.07E+00
1.32E+00
1.91E+00
2.66E+00

7.59E+00
1.25E+01
1.72E+01
2.18E+01
2.62E+01
3.59E+01
4.74E+01

6.89E+00
1.13E+01
1.56E+01
2.02E+01
2.48E+01
3.51E+01
4.60E+01

1.10E+02
1.71E+02
2.21E+02
2.57E+02
2.82E+02
3.16E+02
3.37E+02

1.02E+02
1.57E+02
2.01E+02
2.41E+02
2.68E+02
3.02E+02
3.25E+02

3.84E+02
4.09E+02
4.25E+02
4.41E+02
4.50E+02
4.68E+02
4.82E+02

3.82E+02
4.11E+02
4.35E+02
4.49E+02
4.64E+02
4.88E+02
5.08E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

479
480
481
482
483
484
485
486
487
488
489
490
491
492
493
494
495
496
497
498
499
500
501

Figure A.2. 3 Conversion coefficients from electron fluence to personal dose (ICRP, 2010; Endo,
2017)

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

502
503

Table A.2.4 Conversion coefficients from positron fluence to personal dose (ICRP, 2010; Endo, 2017).
hp() / (pSv cm2)
Ep / MeV
1.0E-02
1.5E-022.0E-02
3.0E-02
4.0E-02
5.0E-02
6.0E-028.0E-02
1.0E-01
1.5E-01
2.0E-01
3.0E-01
4.0E-01
5.0E-01
6.0E-01
8.0E-01
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01
6.0E+01
8.0E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
8.0E+02
1.0E+03

504
505

0
3.28E+00
3.29E+00
3.30E+00
3.33E+00
3.36E+00
3.39E+00
3.42E+00
3.47E+00
3.53E+00
3.67E+00
3.84E+00
4.16E+00
4.52E+00
4.90E+00
5.36E+00
7.41E+00
1.05E+01
1.83E+01
2.57E+01
3.91E+01
5.10E+01
6.17E+01
7.29E+01
9.90E+01
1.26E+02
1.84E+02
2.29E+02
2.94E+02
3.20E+02
3.27E+02
3.33E+02
3.39E+02
3.42E+02
3.49E+02
3.54E+02
3.62E+02
3.66E+02
3.69E+02
3.72E+02
3.76E+02
3.79E+02

max(15) max(30) max(45) max(60) max(75) max(90)
3.14E+00
3.04E+00
2.99E+00
3.01E+00
3.09E+00
3.10E+00
3.12E+00
3.14E+00
3.20E+00
3.35E+00
3.48E+00
3.81E+00
4.16E+00
4.55E+00
5.01E+00
6.81E+00
9.64E+00
1.71E+01
2.43E+01
3.74E+01
4.95E+01
6.08E+01
7.19E+01
9.75E+01
1.25E+02
1.83E+02
2.26E+02
2.91E+02
3.14E+02
3.22E+02
3.27E+02
3.36E+02
3.39E+02
3.48E+02
3.54E+02
3.60E+02
3.64E+02
3.69E+02
3.71E+02
3.76E+02
3.81E+02

2.86E+00
2.74E+00
2.72E+00
2.70E+00
2.79E+00
2.81E+00
2.83E+00
2.85E+00
2.90E+00
3.04E+00
3.18E+00
3.52E+00
3.88E+00
4.32E+00
4.79E+00
6.42E+00
8.87E+00
1.55E+01
2.20E+01
3.40E+01
4.56E+01
5.67E+01
6.79E+01
9.41E+01
1.21E+02
1.77E+02
2.17E+02
2.79E+02
3.10E+02
3.20E+02
3.28E+02
3.36E+02
3.40E+02
3.48E+02
3.54E+02
3.61E+02
3.66E+02
3.72E+02
3.76E+02
3.80E+02
3.83E+02

2.44E+00
2.34E+00
2.30E+00
2.30E+00
2.38E+00
2.39E+00
2.40E+00
2.43E+00
2.46E+00
2.59E+00
2.73E+00
3.04E+00
3.42E+00
3.84E+00
4.31E+00
5.67E+00
7.59E+00
1.30E+01
1.85E+01
2.85E+01
3.86E+01
4.83E+01
5.85E+01
8.45E+01
1.11E+02
1.65E+02
2.03E+02
2.60E+02
2.96E+02
3.13E+02
3.23E+02
3.34E+02
3.39E+02
3.51E+02
3.58E+02
3.69E+02
3.75E+02
3.81E+02
3.85E+02
3.92E+02
3.96E+02

1.99E+00
1.91E+00
1.88E+00
1.88E+00
1.94E+00
1.94E+00
1.95E+00
2.00E+00
2.03E+00
2.15E+00
2.26E+00
2.54E+00
2.84E+00
3.22E+00
3.63E+00
4.71E+00
6.10E+00
1.01E+01
1.43E+01
2.24E+01
3.03E+01
3.82E+01
4.70E+01
6.82E+01
9.09E+01
1.41E+02
1.78E+02
2.33E+02
2.75E+02
3.00E+02
3.17E+02
3.33E+02
3.41E+02
3.57E+02
3.66E+02
3.82E+02
3.90E+02
3.97E+02
4.02E+02
4.14E+02
4.20E+02

1.50E+00
1.45E+00
1.44E+00
1.44E+00
1.49E+00
1.48E+00
1.50E+00
1.54E+00
1.58E+00
1.66E+00
1.75E+00
1.96E+00
2.20E+00
2.45E+00
2.76E+00
3.49E+00
4.44E+00
7.08E+00
9.99E+00
1.59E+01
2.17E+01
2.73E+01
3.37E+01
4.77E+01
6.53E+01
1.05E+02
1.38E+02
1.93E+02
2.47E+02
2.82E+02
3.05E+02
3.28E+02
3.41E+02
3.61E+02
3.74E+02
3.92E+02
4.06E+02
4.17E+02
4.26E+02
4.35E+02
4.48E+02

1.07E+00
1.03E+00
1.03E+00
1.04E+00
1.07E+00
1.08E+00
1.09E+00
1.11E+00
1.14E+00
1.20E+00
1.27E+00
1.42E+00
1.56E+00
1.72E+00
1.90E+00
2.32E+00
2.82E+00
4.28E+00
5.95E+00
9.69E+00
1.36E+01
1.75E+01
2.19E+01
3.14E+01
4.25E+01
7.07E+01
9.26E+01
1.35E+02
1.83E+02
2.28E+02
2.63E+02
3.02E+02
3.26E+02
3.61E+02
3.80E+02
4.09E+02
4.33E+02
4.44E+02
4.60E+02
4.79E+02
4.98E+02

180

ROT

ISO

SS-ISO

IS-ISO

1.62E+00
1.64E+00
1.65E+00
1.68E+00
1.71E+00
1.73E+00
1.76E+00
1.82E+00
1.87E+00
2.01E+00
2.14E+00
2.40E+00
2.65E+00
2.90E+00
3.12E+00
3.32E+00
3.37E+00
3.44E+00
3.59E+00
4.19E+00
5.11E+00
6.31E+00
8.03E+00
1.40E+01
2.36E+01
5.90E+01
1.11E+02
2.21E+02
2.91E+02
3.21E+02
3.34E+02
3.49E+02
3.57E+02
3.71E+02
3.81E+02
3.93E+02
4.02E+02
4.09E+02
4.15E+02
4.24E+02
4.30E+02

1.77E+00
1.71E+00
1.70E+00
1.70E+00
1.75E+00
1.77E+00
1.78E+00
1.82E+00
1.86E+00
1.97E+00
2.07E+00
2.32E+00
2.57E+00
2.84E+00
3.13E+00
3.90E+00
4.94E+00
7.66E+00
1.05E+01
1.59E+01
2.13E+01
2.66E+01
3.23E+01
4.61E+01
5.95E+01
9.55E+01
1.30E+02
1.95E+02
2.42E+02
2.76E+02
2.96E+02
3.20E+02
3.34E+02
3.55E+02
3.68E+02
3.85E+02
3.99E+02
4.08E+02
4.18E+02
4.32E+02
4.36E+02

1.39E+00
1.40E+00
1.41E+00
1.43E+00
1.45E+00
1.47E+00
1.49E+00
1.53E+00
1.57E+00
1.67E+00
1.77E+00
1.98E+00
2.21E+00
2.45E+00
2.72E+00
3.38E+00
4.20E+00
6.42E+00
8.70E+00
1.33E+01
1.80E+01
2.24E+01
2.69E+01
3.67E+01
4.76E+01
7.55E+01
1.04E+02
1.62E+02
2.09E+02
2.43E+02
2.68E+02
3.02E+02
3.23E+02
3.56E+02
3.77E+02
4.05E+02
4.25E+02
4.40E+02
4.53E+02
4.74E+02
4.91E+02

1.45E+00
1.47E+00
1.46E+00
1.49E+00
1.50E+00
1.52E+00
1.57E+00
1.60E+00
1.63E+00
1.72E+00
1.81E+00
2.05E+00
2.28E+00
2.54E+00
2.82E+00
3.51E+00
4.39E+00

1.33E+00
1.33E+00
1.36E+00
1.37E+00
1.40E+00
1.42E+00
1.41E+00
1.46E+00
1.51E+00
1.62E+00
1.73E+00
1.91E+00
2.14E+00
2.36E+00
2.62E+00
3.25E+00
4.01E+00

9.13E+00
1.39E+01
1.88E+01
2.33E+01
2.77E+01
3.77E+01
4.89E+01

8.27E+00
1.27E+01
1.72E+01
2.15E+01
2.61E+01
3.57E+01
4.63E+01

1.08E+02
1.65E+02
2.10E+02
2.44E+02
2.67E+02
3.00E+02
3.19E+02

1.00E+02
1.59E+02
2.08E+02
2.42E+02
2.69E+02
3.04E+02
3.27E+02

3.71E+02
3.98E+02
4.15E+02
4.31E+02
4.44E+02
4.63E+02
4.77E+02

3.83E+02
4.12E+02
4.35E+02
4.49E+02
4.62E+02
4.85E+02
5.05E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

506
507
508
509
510
511
512
513
514
515
516
517
518
519
520
521

Figure A.2.4 Conversion coefficients from positron fluence to personal dose (ICRP, 2010; Endo,2017).

FINAL DRAFT JULY 2017522

NOT TO BE REFERENCED

Table A.2.5 Conversion coefficients from proton fluence to personal dose (ICRP, 2010; Endo, 2017).
hp() / (pSv cm2)
Ep / MeV
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01
6.0E+01
8.0E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
8.0E+02
1.0E+030
5.46E+00
8.20E+00
1.09E+01
1.64E+01
2.19E+01
2.73E+01
3.28E+01
4.37E+01
5.49E+01
1.89E+02
4.28E+02
7.50E+02
1.02E+03
1.18E+03
1.48E+03
2.16E+03
2.51E+03
2.38E+03
1.77E+03
1.38E+03
1.23E+03
1.15E+03
1.16E+03
1.11E+03
1.09E+03

max(15) max(30) max(45) max(60) max(75) max(90)
5.30E+00
7.94E+00
1.06E+01
1.58E+01
2.10E+01
2.61E+01
3.12E+01
4.09E+01
6.37E+01
1.87E+02
4.08E+02
7.31E+02
1.01E+03
1.20E+03
1.47E+03
2.18E+03
2.50E+03
2.40E+03
1.79E+03
1.40E+03
1.25E+03
1.19E+03
1.16E+03
1.13E+03
1.11E+03

5.01E+00
7.50E+00
9.98E+00
1.49E+01
1.97E+01
2.44E+01
2.90E+01
3.77E+01
6.84E+01
1.52E+02
3.59E+02
6.73E+02
9.32E+02
1.18E+03
1.44E+03
2.12E+03
2.37E+03
2.41E+03
1.81E+03
1.40E+03
1.25E+03
1.19E+03
1.18E+03
1.14E+03
1.12E+03

4.53E+00
6.78E+00
9.02E+00
1.34E+01
1.78E+01
2.20E+01
2.60E+01
3.36E+01
6.62E+01
1.33E+02
2.95E+02
5.63E+02
7.81E+02
1.04E+03
1.34E+03
1.95E+03
2.21E+03
2.46E+03
1.84E+03
1.41E+03
1.26E+03
1.21E+03
1.18E+03
1.15E+03
1.14E+03

4.07E+00
6.09E+00
8.10E+00
1.21E+01
1.60E+01
1.98E+01
2.34E+01
3.03E+01
5.84E+01
1.17E+02
2.09E+02
4.30E+02
6.23E+02
8.06E+02
1.10E+03
1.72E+03
1.97E+03
2.31E+03
1.93E+03
1.43E+03
1.28E+03
1.22E+03
1.20E+03
1.18E+03
1.15E+03

3.44E+00
5.16E+00
6.87E+00
1.03E+01
1.36E+01
1.69E+01
2.01E+01
2.64E+01
4.40E+01
8.64E+01
1.47E+02
2.98E+02
4.45E+02
5.54E+02
7.52E+02
1.32E+03
1.58E+03
2.11E+03
2.03E+03
1.44E+03
1.28E+03
1.22E+03
1.20E+03
1.18E+03
1.16E+03

2.81E+00
4.21E+00
5.62E+00
8.43E+00
1.12E+01
1.40E+01
1.68E+01
2.24E+01
2.81E+01
5.07E+01
8.28E+01
1.80E+02
2.90E+02
3.79E+02
5.00E+02
7.99E+02
9.94E+02
1.64E+03
2.18E+03
1.45E+03
1.28E+03
1.21E+03
1.20E+03
1.20E+03
1.20E+03

180

ROT

ISO

SS-ISO

IS-ISO

5.47E+00
8.21E+00
1.09E+01
1.64E+01
2.19E+01
2.73E+01
3.28E+01
4.37E+01
5.46E+01
5.61E+01
4.36E+01
3.61E+01
4.55E+01
7.15E+01
1.56E+02
5.60E+02
1.19E+03
2.82E+03
1.93E+03
1.45E+03
1.30E+03
1.24E+03
1.23E+03
1.23E+03
1.23E+03

4.50E+00
6.75E+00
8.98E+00
1.34E+01
1.78E+01
2.21E+01
2.63E+01
3.45E+01
5.01E+01
9.37E+01
1.65E+02
2.96E+02
4.22E+02
5.32E+02
6.87E+02
1.09E+03
1.44E+03
2.16E+03
1.96E+03
1.44E+03
1.28E+03
1.22E+03
1.22E+03
1.20E+03
1.19E+03

3.52E+00
5.28E+00
7.02E+00
1.05E+01
1.39E+01
1.73E+01
2.05E+01
2.68E+01
4.58E+01
8.01E+01
1.36E+02
2.49E+02
3.58E+02
4.51E+02
5.51E+02
8.37E+02
1.13E+03
1.79E+03
1.84E+03
1.42E+03
1.25E+03
1.18E+03
1.17E+03
1.17E+03
1.15E+03

3.44E+00
5.16E+00
6.86E+00
1.03E+01
1.36E+01
1.69E+01
2.01E+01
2.62E+01
4.66E+01
8.31E+01
1.45E+02
2.66E+02
3.81E+02
4.62E+02
5.47E+02
8.71E+02
1.18E+03
1.85E+03
1.90E+03
1.45E+03
1.28E+03
1.21E+03
1.21E+03
1.18E+03
1.18E+03

3.51E+00
5.26E+00
7.00E+00
1.05E+01
1.39E+01
1.72E+01
2.05E+01
2.67E+01
4.50E+01
7.71E+01
1.27E+02
2.32E+02
3.35E+02
4.40E+02
5.55E+02
8.03E+02
1.08E+03
1.73E+03
1.78E+03
1.39E+03
1.22E+03
1.15E+03
1.13E+03
1.16E+03
1.12E+03

523
524
525
526
527
528
529
530
531
532
533
534
535

Figure A.2.5 Conversion coefficients from proton fluence to personal dose (ICRP, 2010; Endo,2017).

FINAL DRAFT JULY 2017

536
537

NOT TO BE REFERENCED

Table A.2.6 Conversion coefficients from negative muon fluence to personal dose (ICRP, 2010; Endo,2017).
hp() / (pSv cm2)
Ep / MeV
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01
6.0E+01
8.0E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
8.0E+02
1.0E+030
1.80E+02
1.80E+02
1.84E+02
1.88E+02
1.93E+02
2.05E+02
2.42E+02
2.93E+02
3.32E+02
4.14E+02
4.65E+02
6.57E+02
7.35E+02
7.55E+02
6.28E+02
4.31E+02
3.82E+02
3.40E+02
3.26E+02
3.19E+02
3.20E+02
3.21E+02
3.25E+02
3.27E+02
3.33E+02

max(15) max(30) max(45) max(60) max(75) max(90)
1.80E+02
1.82E+02
1.84E+02
1.89E+02
1.95E+02
2.06E+02
2.37E+02
2.83E+02
3.23E+02
4.07E+02
4.68E+02
6.63E+02
7.32E+02
7.63E+02
6.41E+02
4.37E+02
3.90E+02
3.50E+02
3.39E+02
3.36E+02
3.39E+02
3.43E+02
3.46E+02
3.49E+02
3.53E+02

1.65E+02
1.68E+02
1.72E+02
1.75E+02
1.81E+02
1.89E+02
2.12E+02
2.59E+02
2.97E+02
3.76E+02
4.46E+02
6.40E+02
6.96E+02
7.11E+02
6.64E+02
4.50E+02
3.91E+02
3.48E+02
3.38E+02
3.35E+02
3.37E+02
3.41E+02
3.44E+02
3.47E+02
3.52E+02

1.45E+02
1.45E+02
1.48E+02
1.53E+02
1.59E+02
1.69E+02
1.81E+02
2.20E+02
2.52E+02
3.26E+02
4.07E+02
5.92E+02
6.49E+02
6.61E+02
6.73E+02
4.80E+02
3.99E+02
3.53E+02
3.43E+02
3.40E+02
3.42E+02
3.46E+02
3.49E+02
3.52E+02
3.57E+02

1.18E+02
1.19E+02
1.21E+02
1.25E+02
1.29E+02
1.38E+02
1.47E+02
1.73E+02
2.01E+02
2.64E+02
3.29E+02
5.19E+02
5.83E+02
5.99E+02
6.15E+02
5.33E+02
4.08E+02
3.51E+02
3.43E+02
3.38E+02
3.41E+02
3.46E+02
3.48E+02
3.51E+02
3.56E+02

8.86E+01
8.89E+01
9.16E+01
9.38E+01
9.78E+01
1.03E+02
1.10E+02
1.27E+02
1.46E+02
1.92E+02
2.35E+02
3.91E+02
4.71E+02
5.23E+02
5.87E+02
6.02E+02
4.30E+02
3.51E+02
3.42E+02
3.37E+02
3.40E+02
3.44E+02
3.46E+02
3.50E+02
3.54E+02

5.72E+01
5.82E+01
5.86E+01
6.11E+01
6.30E+01
6.59E+01
7.09E+01
7.93E+01
9.33E+01
1.27E+02
1.57E+02
2.51E+02
3.15E+02
3.69E+02
4.56E+02
6.30E+02
4.84E+02
3.64E+02
3.48E+02
3.41E+02
3.44E+02
3.49E+02
3.51E+02
3.55E+02
3.59E+02

180

ROT

ISO

SS-ISO

IS-ISO

7.52E+01
7.68E+01
7.83E+01
8.14E+01
8.48E+01
8.77E+01
8.67E+01
8.68E+01
8.86E+01
1.00E+02
1.22E+02
2.51E+02
4.57E+02
7.03E+02
7.75E+02
4.85E+02
4.02E+02
3.45E+02
3.29E+02
3.21E+02
3.21E+02
3.24E+02
3.26E+02
3.32E+02
3.37E+02

9.75E+01
9.93E+01
1.00E+02
1.04E+02
1.07E+02
1.12E+02
1.22E+02
1.41E+02
1.58E+02
2.00E+02
2.41E+02
3.57E+02
4.62E+02
5.56E+02
5.98E+02
5.29E+02
4.27E+02
3.52E+02
3.39E+02
3.33E+02
3.36E+02
3.41E+02
3.43E+02
3.47E+02
3.51E+02

7.87E+01
7.95E+01
8.09E+01
8.37E+01
8.71E+01
9.15E+01
9.81E+01
1.13E+02
1.27E+02
1.61E+02
1.91E+02
2.75E+02
3.63E+02
4.46E+02
4.96E+02
4.98E+02
4.32E+02
3.54E+02
3.32E+02
3.21E+02
3.21E+02
3.23E+02
3.26E+02
3.31E+02
3.37E+02

8.18E+01
8.28E+01
8.39E+01
8.70E+01
9.06E+01
9.51E+01
1.03E+02
1.18E+02
1.33E+02
1.68E+02
1.97E+02
2.83E+02
3.77E+02
4.64E+02
5.15E+02
5.05E+02
4.35E+02
3.53E+02
3.31E+02
3.20E+02
3.20E+02
3.22E+02
3.24E+02
3.29E+02
3.32E+02

7.56E+01
7.62E+01
7.79E+01
8.04E+01
8.36E+01
8.79E+01
9.32E+01
1.08E+02
1.21E+02
1.54E+02
1.85E+02
2.67E+02
3.49E+02
4.28E+02
4.77E+02
4.91E+02
4.29E+02
3.55E+02
3.33E+02
3.22E+02
3.22E+02
3.24E+02
3.28E+02
3.33E+02
3.42E+02

538
539
540
541
542
543
544
545
546
547
548
549
550
551

Figure A.2.6 Conversion coefficients from negative muon fluence to personal dose (ICRP, 2010;
Endo, 2017)

FINAL DRAFT JULY 2017

552
553

NOT TO BE REFERENCED

Table A.2.7 Conversion coefficients from positive muon fluence to personal dose (ICRP, 2010; Endo,2017).
hp() / (pSv cm2)
Ep / MeV
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01
6.0E+01
8.0E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
8.0E+02
1.0E+030
1.94E+02
1.96E+02
1.98E+02
2.02E+02
2.07E+02
2.16E+02
2.51E+02
3.00E+02
3.40E+02
4.25E+02
4.81E+02
6.74E+02
7.51E+02
7.68E+02
6.35E+02
4.31E+02
3.81E+02
3.39E+02
3.26E+02
3.18E+02
3.19E+02
3.20E+02
3.22E+02
3.25E+02
3.27E+02

max(15) max(30) max(45) max(60) max(75) max(90)
1.81E+02
1.84E+02
1.85E+02
1.91E+02
1.96E+02
2.07E+02
2.37E+02
2.85E+02
3.24E+02
4.08E+02
4.72E+02
6.70E+02
7.37E+02
7.68E+02
6.44E+02
4.37E+02
3.90E+02
3.50E+02
3.39E+02
3.36E+02
3.39E+02
3.43E+02
3.46E+02
3.49E+02
3.53E+02

1.68E+02
1.70E+02
1.72E+02
1.78E+02
1.84E+02
1.92E+02
2.13E+02
2.57E+02
2.95E+02
3.76E+02
4.48E+02
6.46E+02
7.01E+02
7.17E+02
6.66E+02
4.50E+02
3.91E+02
3.48E+02
3.38E+02
3.35E+02
3.37E+02
3.41E+02
3.44E+02
3.47E+02
3.52E+02

1.46E+02
1.48E+02
1.49E+02
1.54E+02
1.60E+02
1.70E+02
1.80E+02
2.19E+02
2.53E+02
3.26E+02
4.10E+02
5.96E+02
6.53E+02
6.65E+02
6.75E+02
4.80E+02
3.99E+02
3.53E+02
3.43E+02
3.39E+02
3.42E+02
3.46E+02
3.49E+02
3.52E+02
3.57E+02

1.20E+02
1.21E+02
1.23E+02
1.28E+02
1.31E+02
1.39E+02
1.48E+02
1.73E+02
2.01E+02
2.67E+02
3.33E+02
5.25E+02
5.88E+02
6.01E+02
6.19E+02
5.34E+02
4.08E+02
3.51E+02
3.42E+02
3.38E+02
3.41E+02
3.46E+02
3.48E+02
3.51E+02
3.56E+02

9.01E+01
9.01E+01
9.18E+01
9.39E+01
9.82E+01
1.04E+02
1.10E+02
1.27E+02
1.45E+02
1.96E+02
2.36E+02
3.94E+02
4.73E+02
5.23E+02
5.90E+02
6.05E+02
4.30E+02
3.51E+02
3.42E+02
3.37E+02
3.40E+02
3.44E+02
3.46E+02
3.50E+02
3.54E+02

5.91E+01
5.99E+01
6.05E+01
6.24E+01
6.43E+01
6.67E+01
7.03E+01
8.04E+01
9.38E+01
1.27E+02
1.60E+02
2.53E+02
3.18E+02
3.71E+02
4.59E+02
6.30E+02
4.83E+02
3.64E+02
3.48E+02
3.41E+02
3.44E+02
3.49E+02
3.51E+02
3.55E+02
3.59E+02

180

ROT

ISO

SS-ISO

IS-ISO

8.26E+01
8.41E+01
8.57E+01
8.89E+01
9.21E+01
9.43E+01
9.25E+01
9.28E+01
9.48E+01
1.08E+02
1.33E+02
2.65E+02
4.73E+02
7.21E+02
7.87E+02
4.83E+02
3.99E+02
3.45E+02
3.28E+02
3.20E+02
3.21E+02
3.23E+02
3.25E+02
3.30E+02
3.33E+02

1.00E+02
1.01E+02
1.02E+02
1.05E+02
1.09E+02
1.14E+02
1.22E+02
1.40E+02
1.58E+02
2.02E+02
2.43E+02
3.61E+02
4.67E+02
5.59E+02
5.99E+02
5.29E+02
4.27E+02
3.52E+02
3.39E+02
3.33E+02
3.36E+02
3.41E+02
3.43E+02
3.46E+02
3.51E+02

8.52E+01
8.62E+01
8.75E+01
9.03E+01
9.36E+01
9.77E+01
1.03E+02
1.17E+02
1.32E+02
1.67E+02
1.99E+02
2.84E+02
3.73E+02
4.56E+02
5.06E+02
5.02E+02
4.32E+02
3.54E+02
3.32E+02
3.20E+02
3.20E+02
3.22E+02
3.24E+02
3.29E+02
3.33E+02

8.89E+01
9.00E+01
9.12E+01
9.40E+01
9.74E+01
1.02E+02
1.08E+02
1.23E+02
1.38E+02
1.74E+02
2.05E+02
2.93E+02
3.89E+02
4.76E+02
5.25E+02
5.10E+02
4.37E+02
3.54E+02
3.31E+02
3.20E+02
3.20E+02
3.22E+02
3.24E+02
3.29E+02
3.32E+02

8.15E+01
8.24E+01
8.38E+01
8.66E+01
8.98E+01
9.34E+01
9.80E+01
1.11E+02
1.26E+02
1.60E+02
1.93E+02
2.75E+02
3.57E+02
4.36E+02
4.87E+02
4.94E+02
4.27E+02
3.54E+02
3.33E+02
3.20E+02
3.20E+02
3.22E+02
3.24E+02
3.29E+02
3.34E+02

554
555
556
557
558
559
560
561
562
563
564
565
566

Figure A.2.7 Conversion coefficients from positive muon fluence to personal dose (ICRP, 2010;
Endo, 2017).

FINAL DRAFT JULY 2017

567
568

NOT TO BE REFERENCED

Table A.2.8 Conversion coefficients from negative pion fluence to personal dose (ICRP, 2010; Endo,2017).
hp() / (pSv cm2)
Ep / MeV
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01
6.0E+01
8.0E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
8.0E+02
1.0E+030
4.06E+02
4.22E+02
4.33E+02
4.58E+02
4.91E+02
5.28E+02
6.73E+02
9.65E+02
1.09E+03
1.25E+03
1.28E+03
1.77E+03
1.92E+03
1.93E+03
1.68E+03
1.14E+03
9.95E+02
9.27E+02
9.02E+02
8.48E+02
8.44E+02
8.69E+02
9.01E+02
9.47E+02
9.77E+02

max(15) max(30) max(45) max(60) max(75) max(90)
4.03E+02
4.24E+02
4.41E+02
4.73E+02
5.15E+02
5.67E+02
6.92E+02
9.84E+02
1.09E+03
1.25E+03
1.35E+03
1.87E+03
1.92E+03
1.93E+03
1.73E+03
1.18E+03
1.04E+03
9.52E+02
9.01E+02
8.66E+02
8.64E+02
8.90E+02
8.96E+02
9.33E+02
9.47E+02

3.75E+02
3.94E+02
4.11E+02
4.46E+02
4.85E+02
5.44E+02
6.29E+02
8.91E+02
1.00E+03
1.16E+03
1.32E+03
1.84E+03
1.85E+03
1.79E+03
1.81E+03
1.21E+03
1.04E+03
9.50E+02
9.04E+02
8.72E+02
8.63E+02
8.88E+02
8.84E+02
9.27E+02
9.40E+02

3.33E+02
3.46E+02
3.61E+02
3.93E+02
4.30E+02
4.82E+02
5.36E+02
7.28E+02
8.23E+02
9.87E+02
1.19E+03
1.69E+03
1.72E+03
1.63E+03
1.63E+03
1.27E+03
1.03E+03
9.48E+02
9.03E+02
8.76E+02
8.70E+02
8.87E+02
8.99E+02
9.42E+02
9.58E+02

2.88E+02
2.98E+02
3.09E+02
3.34E+02
3.64E+02
4.02E+02
4.45E+02
5.35E+02
6.54E+02
8.23E+02
9.40E+02
1.48E+03
1.53E+03
1.50E+03
1.50E+03
1.44E+03
1.05E+03
9.31E+02
8.89E+02
8.65E+02
8.54E+02
8.73E+02
8.94E+02
9.31E+02
9.53E+02

2.29E+02
2.36E+02
2.42E+02
2.58E+02
2.77E+02
3.01E+02
3.29E+02
4.03E+02
4.67E+02
6.03E+02
6.58E+02
1.03E+03
1.24E+03
1.32E+03
1.37E+03
1.47E+03
1.09E+03
9.13E+02
8.72E+02
8.61E+02
8.50E+02
8.71E+02
8.81E+02
9.36E+02
9.42E+02

1.76E+02
1.77E+02
1.79E+02
1.85E+02
1.93E+02
2.00E+02
2.12E+02
2.48E+02
2.89E+02
3.80E+02
4.71E+02
6.54E+02
8.17E+02
8.96E+02
1.01E+03
1.45E+03
1.22E+03
8.81E+02
8.43E+02
8.27E+02
8.33E+02
8.48E+02
8.68E+02
9.01E+02
9.22E+02

180

ROT

ISO

SS-ISO

IS-ISO

1.94E+02
2.01E+02
2.10E+02
2.25E+02
2.33E+02
2.37E+02
2.08E+02
1.81E+02
1.78E+02
1.97E+02
2.44E+02
5.47E+02
1.02E+03
1.70E+03
1.99E+03
1.31E+03
9.91E+02
8.89E+02
8.71E+02
8.43E+02
8.50E+02
8.80E+02
9.17E+02
9.76E+02
1.02E+03

2.45E+02
2.53E+02
2.61E+02
2.80E+02
3.00E+02
3.27E+02
3.59E+02
4.37E+02
4.88E+02
5.81E+02
6.62E+02
9.51E+02
1.18E+03
1.36E+03
1.47E+03
1.36E+03
1.08E+03
9.22E+02
8.71E+02
8.57E+02
8.43E+02
8.63E+02
8.83E+02
9.18E+02
9.38E+02

1.76E+02
1.89E+02
1.98E+02
2.15E+02
2.32E+02
2.51E+02
2.71E+02
3.17E+02
3.61E+02
4.39E+02
5.08E+02
6.76E+02
8.68E+02
1.02E+03
1.15E+03
1.15E+03
1.03E+03
8.57E+02
8.15E+02
7.94E+02
8.07E+02
8.38E+02
8.75E+02
9.35E+02
9.79E+02

1.91E+02
2.06E+02
2.17E+02
2.37E+02
2.55E+02
2.70E+02
3.02E+02
3.52E+02
3.96E+02
4.70E+02
5.31E+02
6.98E+02
9.01E+02
1.07E+03
1.21E+03
1.19E+03
1.03E+03
8.45E+02
8.28E+02
8.06E+02
8.02E+02
8.37E+02
8.90E+02
9.37E+02
9.78E+02

1.61E+02
1.72E+02
1.79E+02
1.93E+02
2.09E+02
2.32E+02
2.40E+02
2.82E+02
3.26E+02
4.08E+02
4.85E+02
6.54E+02
8.35E+02
9.70E+02
1.09E+03
1.11E+03
1.03E+03
8.69E+02
8.02E+02
7.82E+02
8.12E+02
8.39E+02
8.60E+02
9.33E+02
9.80E+02

569
570
571
572
573
574
575
576
577
578
579
580
581

Figure A.2.8 Conversion coefficients from negative pion fluence to personal dose (ICRP, 2010; Endo,2017).

FINAL DRAFT JULY 2017

582
583

NOT TO BE REFERENCED

Table A.2.9 Conversion coefficients from positive pion fluence to personal dose (ICRP, 2010; Endo,2017).
hp() / (pSv cm2)
Ep / MeV
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01
6.0E+01
8.0E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
4.0E+02
5.0E+02
6.0E+02
8.0E+02
1.0E+030
3.14E+02
3.24E+02
3.40E+02
3.79E+02
4.29E+02
4.89E+02
5.40E+02
7.17E+02
8.19E+02
1.00E+03
1.10E+03
1.52E+03
1.75E+03
1.83E+03
1.66E+03
1.22E+03
1.13E+03
1.22E+03
1.25E+03
1.07E+03
9.69E+02
9.43E+02
9.52E+02
9.99E+02
1.04E+03

max(15) max(30) max(45) max(60) max(75) max(90)
2.78E+02
2.90E+02
3.04E+02
3.36E+02
3.80E+02
4.38E+02
4.94E+02
6.51E+02
7.44E+02
9.15E+02
1.04E+03
1.47E+03
1.65E+03
1.71E+03
1.63E+03
1.21E+03
1.11E+03
1.19E+03
1.23E+03
1.08E+03
9.93E+02
9.75E+02
9.64E+02
1.01E+03
1.03E+03

2.57E+02
2.69E+02
2.81E+02
3.10E+02
3.52E+02
4.08E+02
4.53E+02
5.90E+02
6.75E+02
8.40E+02
9.95E+02
1.42E+03
1.58E+03
1.61E+03
1.65E+03
1.24E+03
1.11E+03
1.18E+03
1.23E+03
1.09E+03
9.99E+02
9.75E+02
9.63E+02
1.01E+03
1.03E+03

2.28E+02
2.36E+02
2.48E+02
2.73E+02
3.08E+02
3.54E+02
4.01E+02
4.90E+02
5.68E+02
7.26E+02
8.82E+02
1.30E+03
1.46E+03
1.48E+03
1.50E+03
1.29E+03
1.11E+03
1.17E+03
1.23E+03
1.10E+03
1.01E+03
9.87E+02
9.71E+02
1.03E+03
1.04E+03

1.98E+02
2.04E+02
2.12E+02
2.31E+02
2.57E+02
2.92E+02
3.25E+02
3.84E+02
4.55E+02
5.94E+02
7.06E+02
1.12E+03
1.30E+03
1.35E+03
1.38E+03
1.38E+03
1.11E+03
1.13E+03
1.20E+03
1.10E+03
1.01E+03
9.74E+02
9.66E+02
1.02E+03
1.04E+03

1.59E+02
1.63E+02
1.66E+02
1.80E+02
1.98E+02
2.22E+02
2.40E+02
2.83E+02
3.30E+02
4.31E+02
5.05E+02
7.90E+02
1.03E+03
1.15E+03
1.23E+03
1.37E+03
1.14E+03
1.08E+03
1.17E+03
1.10E+03
1.01E+03
9.73E+02
9.66E+02
1.02E+03
1.03E+03

1.21E+02
1.21E+02
1.22E+02
1.29E+02
1.38E+02
1.53E+02
1.58E+02
1.82E+02
2.12E+02
2.80E+02
3.50E+02
5.14E+02
6.84E+02
7.84E+02
8.99E+02
1.32E+03
1.21E+03
1.02E+03
1.10E+03
1.07E+03
9.92E+02
9.56E+02
9.56E+02
1.00E+03
1.02E+03

180

ROT

ISO

SS-ISO

IS-ISO

1.21E+02
1.25E+02
1.33E+02
1.51E+02
1.70E+02
1.83E+02
1.85E+02
1.77E+02
1.79E+02
2.01E+02
2.47E+02
4.94E+02
9.06E+02
1.48E+03
1.82E+03
1.38E+03
1.12E+03
1.15E+03
1.23E+03
1.10E+03
9.98E+02
9.70E+02
9.80E+02
1.04E+03
1.09E+03

1.65E+02
1.71E+02
1.76E+02
1.91E+02
2.16E+02
2.45E+02
2.64E+02
3.11E+02
3.52E+02
4.38E+02
5.17E+02
7.49E+02
9.77E+02
1.17E+03
1.30E+03
1.30E+03
1.12E+03
1.09E+03
1.18E+03
1.09E+03
1.00E+03
9.75E+02
9.62E+02
1.00E+03
1.03E+03

1.51E+02
1.60E+02
1.68E+02
1.83E+02
1.98E+02
2.16E+02
2.33E+02
2.65E+02
2.96E+02
3.67E+02
4.39E+02
6.02E+02
7.87E+02
9.53E+02
1.09E+03
1.16E+03
1.10E+03
1.05E+03
1.08E+03
1.02E+03
9.53E+02
9.30E+02
9.38E+02
9.93E+02
1.05E+03

1.70E+02
1.82E+02
1.84E+02
2.02E+02
2.20E+02
2.39E+02
2.57E+02
2.93E+02
3.28E+02
3.93E+02
4.66E+02
6.21E+02
8.20E+02
9.93E+02
1.15E+03
1.21E+03
1.10E+03
1.04E+03
1.12E+03
1.04E+03
9.36E+02
9.19E+02
9.44E+02
9.97E+02
1.05E+03

1.32E+02
1.38E+02
1.52E+02
1.64E+02
1.76E+02
1.93E+02
2.09E+02
2.37E+02
2.64E+02
3.41E+02
4.12E+02
5.83E+02
7.54E+02
9.13E+02
1.03E+03
1.11E+03
1.10E+03
1.06E+03
1.04E+03
1.00E+03
9.70E+02
9.41E+02
9.32E+02
9.89E+02
1.05E+03

584
585
586
587
588
589
590
591
592
593
594
595
596

Figure A.2.9 Conversion coefficients from positive pion fluence to personal dose (ICRP, 2010;
Endo, 2017).

FINAL DRAFT JULY 2017

597
598

NOT TO BE REFERENCED

Table A.2.10 Conversion coefficients from helium ion fluence to personal dose (ICRP, 2010; Endo,2017).
hp() / (pSv cm2)Ep /MeV u-10

1.0E+00
2.0E+00
3.0E+00
5.0E+00
1.0E+01
1.4E+01
2.0E+01
3.0E+01
5.0E+01
7.5E+01
1.0E+02
1.5E+02
2.0E+02
3.0E+02
5.0E+02
7.0E+02
1.0E+03

2.19E+02
4.38E+02
6.56E+02
1.09E+03
2.19E+03
4.61E+03
1.72E+04
3.01E+04
4.75E+04
8.05E+04
1.01E+05
9.25E+04
6.74E+04
5.14E+04
4.27E+04
4.11E+04
4.00E+04

max(15) max(30) max(45) max(60) max(75) max(90)
2.12E+02
4.23E+02
6.33E+02
1.04E+03
2.55E+03
5.04E+03
1.62E+04
2.91E+04
4.79E+04
8.04E+04
9.74E+04
9.17E+04
6.81E+04
5.16E+04
4.23E+04
4.00E+04
3.87E+04

2.00E+02
3.99E+02
5.95E+02
9.76E+02
2.73E+03
4.84E+03
1.43E+04
2.68E+04
4.68E+04
7.85E+04
9.26E+04
9.18E+04
6.86E+04
5.15E+04
4.23E+04
3.98E+04
3.84E+04

1.81E+02
3.61E+02
5.38E+02
8.79E+02
2.65E+03
4.67E+03
1.17E+04
2.24E+04
4.14E+04
7.34E+04
8.61E+04
9.32E+04
7.03E+04
5.21E+04
4.26E+04
4.04E+04
3.92E+04

1.63E+02
3.24E+02
4.83E+02
7.90E+02
2.34E+03
4.12E+03
8.33E+03
1.71E+04
3.21E+04
6.46E+04
7.70E+04
8.83E+04
7.32E+04
5.26E+04
4.29E+04
4.08E+04
3.96E+04

1.38E+02
2.75E+02
4.10E+02
6.76E+02
1.76E+03
2.94E+03
5.88E+03
1.19E+04
2.21E+04
4.68E+04
6.14E+04
8.04E+04
7.59E+04
5.23E+04
4.25E+04
4.07E+04
3.97E+04

1.10E+02
2.20E+02
3.30E+02
5.50E+02
1.10E+03
1.62E+03
3.27E+03
7.07E+03
1.51E+04
2.81E+04
3.88E+04
6.31E+04
8.26E+04
5.31E+04
4.25E+04
4.04E+04
3.91E+04

180

ROT

ISO

SS-ISO

IS-ISO

2.19E+02
4.38E+02
6.57E+02
1.09E+03
2.19E+03
2.56E+03
1.74E+03
1.44E+03
2.88E+03
1.75E+04
4.84E+04
1.10E+05
7.29E+04
5.33E+04
4.49E+04
4.60E+04
4.47E+04

1.76E+02
3.52E+02
5.26E+02
8.66E+02
1.97E+03
3.09E+03
6.56E+03
1.18E+04
2.15E+04
3.94E+04
5.64E+04
8.26E+04
7.36E+04
5.22E+04
4.23E+04
4.03E+04
3.92E+04

1.41E+02
2.81E+02
4.19E+02
6.89E+02
1.82E+03
2.81E+03
5.46E+03
9.86E+03
1.78E+04
3.00E+04
4.55E+04
6.95E+04
7.01E+04
5.25E+04
4.27E+04
4.19E+04
4.09E+04

1.38E+02
2.75E+02
4.10E+02
6.74E+02
1.86E+03
2.95E+03
5.73E+03
1.04E+04
1.86E+04
3.11E+04
4.62E+04
7.21E+04
7.20E+04
5.33E+04
4.27E+04
4.04E+04
3.89E+04

1.40E+02
2.80E+02
4.18E+02
6.87E+02
1.73E+03
2.64E+03
5.02E+03
9.15E+03
1.71E+04
2.91E+04
4.23E+04
6.61E+04
6.90E+04
5.22E+04
4.20E+04
4.03E+04
3.94E+04

599
600
601
602
603
604
605
606
607
608
609
610
611
612
613

Figure A.2.10 Conversion coefficients from helium ion fluence to personal dose (ICRP, 2010;
Endo, 2017).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

614
615

A.3 Directional and Personal Absorbed Dose to the Lens of the Eye

616

The numerical values of conversion coefficients from particle fluence to directional absorbed

617

dose in the lens of the eye d'lens and from fluence to personal absorbed dose in the lens of the eye

618

dplens are the same and the symbol dlens, is used in the following Tables. The conversion coefficients

619

given here are to the value of the absorbed dose in the lens of the eye calculated for whole-body620

exposure of the stylized eye model (Behrens and Dietze, 2011) for broad parallel beams incident for

621

angles, α, from 0° (A-P) to 90° in 15° steps. The maximum value of absorbed dose is taken for right622

or left irradiations; and for a rotational field.

623

Tables A.3.1a to A.3.4 and Figures A.3.1a to A.3.4 give the numerical values of the conversion

624

coefficients for energies up to 50 MeV from particle fluence for photons, neutrons, electrons, and625

positrons; and Table A.3.1b and Figure A.3.1b for photons from air kerma.

626

FINAL DRAFT JULY 2017

627
628

NOT TO BE REFERENCED

Table A.3.1a Conversion coefficients from photon fluence to the maximum absorbed dose in thecomplete lens for left or right irradiations (Behrens, 2017a).
dlens(α)/ (pGy cm2)for a radiation incidence at 
Ep / MeV
0.005
0.006
0.007
0.008
0.009
0.01
0.011
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.12
0.15
0.2
0.24
0.3
0.4
0.5
0.511
0.6
0.662
0.8
1
1.117
1.2
1.3
1.33
1.5
1.7
2
2.4
3
4
5
6
6.129
8
10
15
20
30
40
50

0

15

30

45

60

75

90

ROT

8.61E-06
2.00E-03
3.74E-02
1.85E-01
4.75E-01
8.33E-01
1.15E+00
1.54E+00
1.63E+00
1.55E+00
1.35E+00
1.09E+00
8.12E-01
5.80E-01
4.83E-01
4.50E-01
4.55E-01
4.82E-01
5.59E-01
6.63E-01
8.38E-01
1.13E+00
1.38E+00
1.74E+00
2.29E+00
2.83E+00
2.88E+00
3.34E+00
3.63E+00
4.26E+00
5.06E+00
5.50E+00
5.83E+00
6.07E+00
6.16E+00
6.59E+00
6.92E+00
7.04E+00
6.84E+00
6.35E+00
5.62E+00
5.13E+00
4.82E+00
4.79E+00
4.42E+00
4.17E+00
3.97E+00
3.94E+00
4.01E+00
4.09E+00
4.16E+00

1.63E-05
2.44E-03
3.56E-02
1.72E-01
4.41E-01
7.78E-01
1.10E+00
1.52E+00
1.63E+00
1.57E+00
1.37E+00
1.11E+00
8.35E-01
5.93E-01
4.94E-01
4.59E-01
4.63E-01
4.83E-01
5.62E-01
6.66E-01
8.40E-01
1.15E+00
1.38E+00
1.75E+00
2.32E+00
2.84E+00
2.88E+00
3.36E+00
3.65E+00
4.28E+00
5.09E+00
5.55E+00
5.84E+00
6.14E+00
6.26E+00
6.63E+00
6.93E+00
7.16E+00
6.93E+00
6.49E+00
5.85E+00
5.35E+00
5.05E+00
5.06E+00
4.67E+00
4.38E+00
4.16E+00
4.08E+00
4.12E+00
4.18E+00
4.32E+00

3.47E-05
2.97E-03
3.67E-02
1.63E-01
4.13E-01
7.30E-01
1.04E+00
1.46E+00
1.58E+00
1.54E+00
1.36E+00
1.11E+00
8.34E-01
6.01E-01
5.04E-01
4.67E-01
4.67E-01
4.89E-01
5.69E-01
6.72E-01
8.46E-01
1.16E+00
1.41E+00
1.77E+00
2.34E+00
2.89E+00
2.97E+00
3.40E+00
3.66E+00
4.33E+00
5.14E+00
5.56E+00
5.86E+00
6.16E+00
6.26E+00
6.71E+00
7.08E+00
7.29E+00
7.24E+00
6.92E+00
6.43E+00
6.08E+00
5.87E+00
5.76E+00
5.52E+00
5.19E+00
4.78E+00
4.60E+00
4.58E+00
4.68E+00
4.71E+00

3.29E-05
2.85E-03
3.38E-02
1.50E-01
3.77E-01
6.72E-01
9.66E-01
1.35E+00
1.49E+00
1.46E+00
1.30E+00
1.07E+00
8.13E-01
5.89E-01
4.96E-01
4.64E-01
4.63E-01
4.85E-01
5.71E-01
6.73E-01
8.45E-01
1.17E+00
1.42E+00
1.80E+00
2.38E+00
2.93E+00
3.01E+00
3.46E+00
3.77E+00
4.39E+00
5.27E+00
5.65E+00
5.98E+00
6.35E+00
6.40E+00
6.88E+00
7.25E+00
7.66E+00
7.84E+00
7.87E+00
7.67E+00
7.68E+00
7.60E+00
7.62E+00
7.47E+00
7.16E+00
6.58E+00
6.15E+00
5.84E+00
5.69E+00
5.70E+00

1.35E-05
1.48E-03
2.02E-02
9.81E-02
2.66E-01
5.07E-01
7.72E-01
1.19E+00
1.37E+00
1.39E+00
1.27E+00
1.06E+00
8.13E-01
5.92E-01
4.95E-01
4.61E-01
4.61E-01
4.90E-01
5.70E-01
6.71E-01
8.45E-01
1.15E+00
1.39E+00
1.75E+00
2.35E+00
2.90E+00
2.98E+00
3.41E+00
3.70E+00
4.37E+00
5.21E+00
5.64E+00
5.95E+00
6.30E+00
6.45E+00
6.91E+00
7.40E+00
7.92E+00
8.47E+00
8.99E+00
9.64E+00
1.01E+01
1.07E+01
1.08E+01
1.16E+01
1.22E+01
1.25E+01
1.24E+01
1.19E+01
1.17E+01
1.16E+01

1.66E-06
4.08E-04
7.75E-03
4.70E-02
1.50E-01
3.20E-01
5.35E-01
9.32E-01
1.16E+00
1.23E+00
1.16E+00
9.98E-01
7.80E-01
5.69E-01
4.76E-01
4.50E-01
4.53E-01
4.79E-01
5.57E-01
6.63E-01
8.36E-01
1.14E+00
1.38E+00
1.75E+00
2.31E+00
2.84E+00
2.89E+00
3.36E+00
3.65E+00
4.28E+00
5.08E+00
5.56E+00
5.82E+00
6.15E+00
6.29E+00
6.74E+00
7.23E+00
7.88E+00
8.64E+00
9.61E+00
1.09E+01
1.22E+01
1.34E+01
1.34E+01
1.56E+01
1.76E+01
2.08E+01
2.29E+01
2.46E+01
2.55E+01
2.64E+01

6.90E-08
4.26E-05
1.75E-03
1.47E-02
5.89E-02
1.52E-01
2.89E-01
5.98E-01
8.31E-01
9.53E-01
9.65E-01
8.69E-01
6.99E-01
5.29E-01
4.47E-01
4.28E-01
4.33E-01
4.58E-01
5.41E-01
6.43E-01
8.11E-01
1.13E+00
1.37E+00
1.73E+00
2.32E+00
2.83E+00
2.89E+00
3.35E+00
3.64E+00
4.27E+00
5.12E+00
5.57E+00
5.92E+00
6.20E+00
6.29E+00
6.83E+00
7.37E+00
8.05E+00
8.74E+00
9.32E+00
1.10E+01
1.26E+01
1.40E+01
1.43E+01
1.71E+01
1.95E+01
2.57E+01
3.09E+01
3.79E+01
4.22E+01
4.53E+01

8.85E-06
8.75E-04
1.24E-02
5.81E-02
1.50E-01
2.74E-01
3.98E-01
5.80E-01
6.57E-01
6.66E-01
6.19E-01
5.35E-01
4.34E-01
3.36E-01
2.95E-01
2.85E-01
2.94E-01
3.15E-01
3.76E-01
4.52E-01
5.80E-01
8.10E-01
1.00E+00
1.28E+00
1.75E+00
2.22E+00
2.26E+00
2.64E+00
2.90E+00
3.46E+00
4.20E+00
4.63E+00
4.87E+00
5.18E+00
5.25E+00
5.76E+00
6.20E+00
6.75E+00
7.32E+00
7.86E+00
8.63E+00
9.35E+00
9.99E+00
1.01E+01
1.14E+01
1.27E+01
1.58E+01
1.89E+01
2.45E+01
2.95E+01
3.36E+01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

629
630
631
632
633
634
635
636
637
638
639
640
641
642
643
644
645
646

Figure A.3.1a Conversion coefficients from photon fluence to the maximum absorbed dose in
the complete lens for left or right irradiations (Behrens, 2017a).

FINAL DRAFT JULY 2017

647
648

NOT TO BE REFERENCED

Table A.3.1b Conversion coefficients from photon air kerma to the maximum absorbed dose in thecomplete lens for left or right irradiations (Behrens, 2017a).
dlens(α)/ (Gy Gy-1) for a radiation incidence at 
Ep / MeV
0.005
0.006
0.007
0.008
0.009
0.01
0.011
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.12
0.15
0.2
0.24
0.3
0.4
0.5
0.511
0.6
0.662
0.8
1
1.117
1.2
1.3
1.33
1.5
1.7
2
2.4
3
4
5
6
6.129
8
10
15
20
30
40
50

0
2.81E-07
9.41E-05
2.41E-03
1.57E-02
5.15E-02
1.13E-01
1.91E-01
3.63E-01
5.20E-01
6.49E-01
7.99E-01
9.47E-01
1.12E+00
1.35E+00
1.50E+00
1.56E+00
1.58E+00
1.57E+00
1.51E+00
1.44E+00
1.40E+00
1.32E+00
1.30E+00
1.26E+00
1.21E+00
1.19E+00
1.18E+00
1.18E+00
1.17E+00
1.15E+00
1.13E+00
1.13E+00
1.13E+00
1.10E+00
1.10E+00
1.07E+00
1.03E+00
9.32E-01
7.99E-01
6.36E-01
4.63E-01
3.62E-01
2.98E-01
2.92E-01
2.20E-01
1.73E-01
1.15E-01
8.69E-02
5.84E-02
4.39E-02
3.49E-0215
5.30E-07
1.15E-04
2.29E-03
1.46E-02
4.78E-02
1.05E-01
1.82E-01
3.59E-01
5.21E-01
6.58E-01
8.15E-01
9.64E-01
1.16E+00
1.38E+00
1.53E+00
1.59E+00
1.61E+00
1.58E+00
1.51E+00
1.45E+00
1.40E+00
1.34E+00
1.30E+00
1.26E+00
1.23E+00
1.19E+00
1.18E+00
1.18E+00
1.17E+00
1.16E+00
1.13E+00
1.14E+00
1.13E+00
1.12E+00
1.12E+00
1.08E+00
1.03E+00
9.48E-01
8.10E-01
6.51E-01
4.82E-01
3.77E-01
3.12E-01
3.08E-01
2.32E-01
1.81E-01
1.21E-01
9.00E-02
6.00E-02
4.48E-02
3.62E-0230
1.13E-06
1.40E-04
2.37E-03
1.38E-02
4.47E-02
9.87E-02
1.72E-01
3.44E-01
5.07E-01
6.43E-01
8.07E-01
9.67E-01
1.16E+00
1.40E+00
1.56E+00
1.62E+00
1.62E+00
1.59E+00
1.53E+00
1.46E+00
1.41E+00
1.36E+00
1.32E+00
1.28E+00
1.24E+00
1.21E+00
1.22E+00
1.20E+00
1.18E+00
1.17E+00
1.15E+00
1.14E+00
1.14E+00
1.12E+00
1.12E+00
1.09E+00
1.05E+00
9.64E-01
8.46E-01
6.93E-01
5.29E-01
4.29E-01
3.63E-01
3.50E-01
2.74E-01
2.15E-01
1.39E-01
1.01E-01
6.68E-02
5.01E-02
3.95E-0245
1.07E-06
1.34E-04
2.18E-03
1.27E-02
4.09E-02
9.09E-02
1.60E-01
3.20E-01
4.76E-01
6.11E-01
7.71E-01
9.29E-01
1.13E+00
1.37E+00
1.54E+00
1.61E+00
1.61E+00
1.58E+00
1.54E+00
1.46E+00
1.41E+00
1.37E+00
1.33E+00
1.31E+00
1.26E+00
1.23E+00
1.24E+00
1.22E+00
1.21E+00
1.19E+00
1.18E+00
1.16E+00
1.16E+00
1.16E+00
1.14E+00
1.12E+00
1.08E+00
1.01E+00
9.16E-01
7.89E-01
6.32E-01
5.41E-01
4.70E-01
4.63E-01
3.71E-01
2.97E-01
1.91E-01
1.35E-01
8.51E-02
6.10E-02
4.79E-0260
4.39E-07
6.97E-05
1.30E-03
8.32E-03
2.89E-02
6.85E-02
1.28E-01
2.82E-01
4.40E-01
5.82E-01
7.55E-01
9.21E-01
1.13E+00
1.38E+00
1.53E+00
1.60E+00
1.60E+00
1.60E+00
1.54E+00
1.46E+00
1.41E+00
1.34E+00
1.31E+00
1.27E+00
1.24E+00
1.22E+00
1.23E+00
1.20E+00
1.19E+00
1.18E+00
1.16E+00
1.15E+00
1.15E+00
1.15E+00
1.15E+00
1.12E+00
1.10E+00
1.05E+00
9.89E-01
9.02E-01
7.94E-01
7.15E-01
6.62E-01
6.55E-01
5.74E-01
5.06E-01
3.62E-01
2.74E-01
1.74E-01
1.26E-01
9.77E-0275
5.42E-08
1.92E-05
5.00E-04
3.98E-03
1.63E-02
4.33E-02
8.86E-02
2.20E-01
3.72E-01
5.15E-01
6.91E-01
8.67E-01
1.08E+00
1.33E+00
1.48E+00
1.56E+00
1.58E+00
1.56E+00
1.50E+00
1.44E+00
1.39E+00
1.33E+00
1.30E+00
1.26E+00
1.22E+00
1.19E+00
1.19E+00
1.18E+00
1.17E+00
1.15E+00
1.13E+00
1.14E+00
1.13E+00
1.12E+00
1.12E+00
1.10E+00
1.08E+00
1.04E+00
1.01E+00
9.63E-01
9.01E-01
8.61E-01
8.30E-01
8.13E-01
7.73E-01
7.28E-01
6.04E-01
5.04E-01
3.59E-01
2.73E-01
2.21E-0190
2.25E-09
2.01E-06
1.13E-04
1.24E-03
6.39E-03
2.06E-02
4.78E-02
1.41E-01
2.66E-01
3.99E-01
5.73E-01
7.56E-01
9.69E-01
1.23E+00
1.38E+00
1.48E+00
1.51E+00
1.49E+00
1.46E+00
1.40E+00
1.35E+00
1.32E+00
1.29E+00
1.25E+00
1.23E+00
1.19E+00
1.19E+00
1.18E+00
1.17E+00
1.15E+00
1.14E+00
1.14E+00
1.15E+00
1.13E+00
1.12E+00
1.11E+00
1.10E+00
1.07E+00
1.02E+00
9.35E-01
9.04E-01
8.89E-01
8.68E-01
8.69E-01
8.47E-01
8.07E-01
7.47E-01
6.81E-01
5.53E-01
4.52E-01
3.80E-01

ROT
2.89E-07
4.12E-05
7.99E-04
4.92E-03
1.63E-02
3.70E-02
6.59E-02
1.37E-01
2.10E-01
2.79E-01
3.68E-01
4.66E-01
6.02E-01
7.85E-01
9.12E-01
9.86E-01
1.02E+00
1.03E+00
1.01E+00
9.81E-01
9.67E-01
9.45E-01
9.44E-01
9.28E-01
9.27E-01
9.31E-01
9.28E-01
9.28E-01
9.31E-01
9.35E-01
9.36E-01
9.48E-01
9.42E-01
9.43E-01
9.39E-01
9.37E-01
9.22E-01
8.93E-01
8.54E-01
7.88E-01
7.11E-01
6.60E-01
6.18E-01
6.15E-01
5.67E-01
5.26E-01
4.59E-01
4.17E-01
3.57E-01
3.16E-01
2.82E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

649
650
651
652
653
654
655
656
657
658
659
660
661
662
663
664
665
666
667

Figure A.3.1b Conversion coefficients from photon air kerma to the maximum absorbed dose in
the complete lens for left or right irradiations (Behrens, 2017a).

FINAL DRAFT JULY 2017

668
669
670

Table A.3.2 and Figure A.3.2 Neutrons

NOT TO BE REFERENCED

FINAL DRAFT JULY 2017

671
672

NOT TO BE REFERENCED

Table A.3.3 Conversion coefficients from electron fluence to the maximum absorbed dose in thecomplete lens for left or right irradiations (Behrens, 2017a).
dlens(α )/ (pGy cm2) for a radiation incidence at 
Ep / MeV
0.01
0.015
0.02
0.03
0.04
0.05
0.06
0.08
0.1
0.15
0.2
0.3
0.4
0.5
0.6
0.7
0.8
1
1.25
1.5
1.75
2
2.5
3
3.5
4
5
6
7
8
10
15
20
30
40
50

673

0

15

30

45

60

75

90

ROT

6.50E-07
1.55E-05
5.26E-05
1.62E-04
3.16E-04
4.90E-04
6.27E-04
1.03E-03
1.43E-03
2.60E-03
3.87E-03
7.36E-03
1.14E-02
1.65E-02
4.71E-02
1.46E+00
1.00E+01
6.95E+01
1.92E+02
3.08E+02
3.85E+02
4.16E+02
4.08E+02
3.78E+02
3.54E+02
3.39E+02
3.23E+02
3.15E+02
3.10E+02
3.07E+02
3.04E+02
3.01E+02
3.01E+02
3.03E+02
3.03E+02
3.00E+02

7.33E-07
1.47E-05
5.21E-05
1.69E-04
3.04E-04
5.09E-04
6.42E-04
1.05E-03
1.47E-03
2.66E-03
4.05E-03
7.18E-03
1.15E-02
1.63E-02
5.68E-02
1.65E+00
1.03E+01
6.74E+01
1.85E+02
2.99E+02
3.78E+02
4.12E+02
4.12E+02
3.87E+02
3.66E+02
3.51E+02
3.35E+02
3.28E+02
3.22E+02
3.18E+02
3.12E+02
3.06E+02
3.03E+02
3.04E+02
3.07E+02
3.01E+02

6.46E-07
1.37E-05
4.29E-05
1.52E-04
3.07E-04
4.76E-04
6.12E-04
9.82E-04
1.34E-03
2.48E-03
3.76E-03
6.86E-03
1.08E-02
1.56E-02
6.98E-02
1.88E+00
1.04E+01
6.02E+01
1.64E+02
2.69E+02
3.50E+02
3.95E+02
4.13E+02
3.99E+02
3.82E+02
3.69E+02
3.54E+02
3.49E+02
3.46E+02
3.41E+02
3.30E+02
3.09E+02
3.05E+02
3.06E+02
3.03E+02
3.06E+02

4.68E-07
1.20E-05
4.00E-05
1.37E-04
2.53E-04
3.94E-04
5.17E-04
8.34E-04
1.26E-03
2.14E-03
3.39E-03
6.29E-03
1.02E-02
1.44E-02
6.62E-02
1.73E+00
9.08E+00
4.86E+01
1.32E+02
2.23E+02
3.02E+02
3.58E+02
4.04E+02
4.11E+02
4.05E+02
3.99E+02
3.92E+02
3.94E+02
4.01E+02
4.06E+02
4.03E+02
3.53E+02
3.23E+02
3.12E+02
3.13E+02
3.10E+02

3.82E-07
1.10E-05
3.07E-05
9.59E-05
1.99E-04
3.45E-04
4.43E-04
7.25E-04
1.01E-03
1.79E-03
2.81E-03
5.15E-03
8.49E-03
1.22E-02
4.51E-02
1.17E+00
6.28E+00
3.36E+01
9.15E+01
1.61E+02
2.28E+02
2.83E+02
3.52E+02
3.82E+02
3.91E+02
3.87E+02
3.68E+02
3.49E+02
3.37E+02
3.28E+02
3.44E+02
4.15E+02
4.03E+02
3.67E+02
3.47E+02
3.41E+02

2.91E-07
6.71E-06
2.01E-05
7.96E-05
1.55E-04
2.36E-04
3.05E-04
5.15E-04
7.44E-04
1.37E-03
2.18E-03
4.07E-03
6.68E-03
9.69E-03
2.34E-02
5.49E-01
3.28E+00
1.89E+01
5.38E+01
9.82E+01
1.46E+02
1.93E+02
2.70E+02
3.21E+02
3.52E+02
3.70E+02
3.81E+02
3.76E+02
3.64E+02
3.53E+02
3.36E+02
3.15E+02
3.76E+02
3.67E+02
3.46E+02
3.32E+02

1.67E-07
3.99E-06
1.56E-05
4.59E-05
8.87E-05
1.44E-04
1.93E-04
3.28E-04
4.96E-04
9.10E-04
1.43E-03
2.84E-03
4.73E-03
6.87E-03
1.16E-02
1.73E-01
1.18E+00
7.80E+00
2.43E+01
4.72E+01
7.39E+01
1.03E+02
1.62E+02
2.11E+02
2.54E+02
2.86E+02
3.33E+02
3.61E+02
3.75E+02
3.76E+02
3.61E+02
3.25E+02
3.12E+02
3.09E+02
3.13E+02
3.13E+02

3.32E-07
4.60E-06
1.69E-05
5.49E-05
9.57E-05
1.56E-04
2.19E-04
3.51E-04
4.84E-04
9.40E-04
1.44E-03
2.63E-03
4.19E-03
6.38E-03
2.29E-02
5.98E-01
3.45E+00
2.08E+01
5.71E+01
9.53E+01
1.26E+02
1.45E+02
1.61E+02
1.64E+02
1.64E+02
1.64E+02
1.65E+02
1.68E+02
1.72E+02
1.77E+02
1.85E+02
2.01E+02
2.12E+02
2.36E+02
2.64E+02
2.90E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

674
675
676
677
678
679
680
681
682
683
684
685
686
687
688
689
690
691
692
693

Figure A.3.3 Conversion coefficients from electrons fluence to the maximum absorbed dose in
the complete lens for left or right irradiations (Behrens, 2017a).

FINAL DRAFT JULY 2017

694
695

NOT TO BE REFERENCED

Table A.3.4 Conversion coefficients from positron fluence to the maximum absorbed dose in thecomplete lens for left or right irradiations (Behrens, 2017a).
dlens(α )/ (pGy cm2) for a radiation incidence at 
Ep / MeV
0.001
0.002
0.003
0.004
0.005
0.006
0.007
0.008
0.009
0.01
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.15
0.2
0.3
0.4
0.5
0.6
0.7
0.8
1
1.25
1.5
1.75
2
2.5
3
3.5
4
5
6
7
8
10
15
20
30
40
50

696

0

15

30

45

60

75

90

ROT

6.79E+00
6.47E+00
6.32E+00
6.29E+00
6.30E+00
6.26E+00
6.27E+00
6.26E+00
6.25E+00
6.26E+00
6.25E+00
6.24E+00
6.23E+00
6.23E+00
6.27E+00
6.26E+00
6.26E+00
6.29E+00
6.26E+00
6.29E+00
6.26E+00
6.30E+00
6.36E+00
6.43E+00
6.56E+00
6.76E+00
6.98E+00
7.31E+00
9.18E+00
1.89E+01
8.22E+01
2.05E+02
3.17E+02
3.84E+02
4.06E+02
3.88E+02
3.59E+02
3.38E+02
3.22E+02
3.10E+02
3.05E+02
3.00E+02
2.99E+02
2.96E+02
2.97E+02
2.98E+02
2.99E+02
2.99E+02
3.02E+02

7.16E+00
6.82E+00
6.68E+00
6.65E+00
6.62E+00
6.61E+00
6.67E+00
6.66E+00
6.65E+00
6.63E+00
6.65E+00
6.66E+00
6.59E+00
6.58E+00
6.64E+00
6.59E+00
6.55E+00
6.62E+00
6.58E+00
6.66E+00
6.64E+00
6.66E+00
6.68E+00
6.78E+00
6.93E+00
7.11E+00
7.36E+00
7.60E+00
9.70E+00
1.94E+01
8.02E+01
1.99E+02
3.07E+02
3.77E+02
4.03E+02
3.94E+02
3.69E+02
3.47E+02
3.36E+02
3.22E+02
3.17E+02
3.12E+02
3.06E+02
3.02E+02
3.01E+02
2.99E+02
2.99E+02
3.03E+02
3.00E+02

7.32E+00
6.92E+00
6.79E+00
6.78E+00
6.75E+00
6.71E+00
6.70E+00
6.65E+00
6.71E+00
6.71E+00
6.67E+00
6.65E+00
6.71E+00
6.69E+00
6.70E+00
6.66E+00
6.73E+00
6.66E+00
6.68E+00
6.75E+00
6.73E+00
6.70E+00
6.79E+00
6.85E+00
7.02E+00
7.16E+00
7.42E+00
7.67E+00
9.91E+00
1.96E+01
7.23E+01
1.76E+02
2.78E+02
3.51E+02
3.87E+02
3.97E+02
3.78E+02
3.65E+02
3.53E+02
3.42E+02
3.38E+02
3.34E+02
3.32E+02
3.23E+02
3.06E+02
3.01E+02
3.00E+02
3.03E+02
3.03E+02

6.78E+00
6.44E+00
6.30E+00
6.27E+00
6.27E+00
6.25E+00
6.23E+00
6.23E+00
6.23E+00
6.18E+00
6.23E+00
6.19E+00
6.20E+00
6.18E+00
6.21E+00
6.19E+00
6.19E+00
6.22E+00
6.28E+00
6.18E+00
6.26E+00
6.27E+00
6.28E+00
6.43E+00
6.46E+00
6.57E+00
6.75E+00
7.04E+00
9.15E+00
1.73E+01
5.91E+01
1.44E+02
2.32E+02
3.07E+02
3.53E+02
3.89E+02
3.96E+02
3.85E+02
3.81E+02
3.74E+02
3.80E+02
3.84E+02
3.91E+02
3.88E+02
3.40E+02
3.16E+02
3.07E+02
3.03E+02
3.02E+02

5.84E+00
5.51E+00
5.38E+00
5.37E+00
5.33E+00
5.24E+00
5.28E+00
5.31E+00
5.30E+00
5.33E+00
5.26E+00
5.31E+00
5.30E+00
5.28E+00
5.30E+00
5.26E+00
5.28E+00
5.31E+00
5.28E+00
5.31E+00
5.31E+00
5.36E+00
5.35E+00
5.46E+00
5.48E+00
5.62E+00
5.82E+00
5.95E+00
7.40E+00
1.31E+01
4.20E+01
1.03E+02
1.70E+02
2.35E+02
2.88E+02
3.49E+02
3.69E+02
3.73E+02
3.68E+02
3.49E+02
3.36E+02
3.25E+02
3.16E+02
3.33E+02
3.94E+02
3.86E+02
3.53E+02
3.40E+02
3.31E+02

4.70E+00
4.37E+00
4.26E+00
4.21E+00
4.18E+00
4.17E+00
4.15E+00
4.14E+00
4.16E+00
4.18E+00
4.12E+00
4.13E+00
4.12E+00
4.15E+00
4.16E+00
4.10E+00
4.14E+00
4.12E+00
4.14E+00
4.20E+00
4.15E+00
4.13E+00
4.15E+00
4.24E+00
4.34E+00
4.41E+00
4.45E+00
4.67E+00
5.37E+00
8.52E+00
2.51E+01
6.13E+01
1.05E+02
1.52E+02
1.98E+02
2.66E+02
3.12E+02
3.40E+02
3.55E+02
3.65E+02
3.60E+02
3.46E+02
3.38E+02
3.23E+02
3.09E+02
3.58E+02
3.47E+02
3.30E+02
3.23E+02

3.40E+00
3.11E+00
3.01E+00
2.95E+00
2.94E+00
2.88E+00
2.91E+00
2.93E+00
2.89E+00
2.86E+00
2.89E+00
2.89E+00
2.91E+00
2.92E+00
2.88E+00
2.88E+00
2.85E+00
2.89E+00
2.88E+00
2.91E+00
2.91E+00
2.90E+00
2.93E+00
2.94E+00
2.98E+00
3.07E+00
3.16E+00
3.25E+00
3.51E+00
4.68E+00
1.20E+01
2.90E+01
5.25E+01
7.86E+01
1.08E+02
1.65E+02
2.12E+02
2.48E+02
2.78E+02
3.23E+02
3.48E+02
3.59E+02
3.61E+02
3.44E+02
3.17E+02
3.05E+02
3.03E+02
3.01E+02
3.03E+02

2.83E+00
2.65E+00
2.59E+00
2.59E+00
2.55E+00
2.52E+00
2.52E+00
2.52E+00
2.54E+00
2.52E+00
2.51E+00
2.52E+00
2.50E+00
2.52E+00
2.51E+00
2.51E+00
2.50E+00
2.53E+00
2.51E+00
2.53E+00
2.53E+00
2.51E+00
2.56E+00
2.58E+00
2.67E+00
2.72E+00
2.80E+00
2.91E+00
3.68E+00
6.87E+00
2.53E+01
6.24E+01
9.91E+01
1.27E+02
1.44E+02
1.57E+02
1.59E+02
1.57E+02
1.58E+02
1.60E+02
1.63E+02
1.67E+02
1.70E+02
1.80E+02
1.94E+02
2.07E+02
2.31E+02
2.60E+02
2.83E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

697
698
699
700
701
702
703
704
705
706
707
708
709
710
711
712
713
714
715

Figure A.3.4 Conversion coefficients from positron fluence to the maximum absorbed dosein the complete lens for left or right irradiations (Behrens, 2017a).

FINAL DRAFT JULY 2017

716

A.4

NOT TO BE REFERENCED

Directional and Personal Absorbed Dose to Local Skin

717

The numerical values of conversion coefficients from particle fluence to directional absorbed

718

dose in local skin d'local skin and from particle fluence to personal absorbed dose in local skin dp local skin719

are the same for exposure of a specific phantom. The symbol dlocal skin is used in the following Tables

720

for the slab phantom. Tables A.4.1.1a, A.4.1.2a, A.4.1.3a, A.4.4, A.4.5 and Figures A.4.1.1a,

721

A.4.1.2a, A.4.1.3a, A.4.4, A.4.5 give the values of the conversion coefficients from particle fluence722

for photons, neutrons, electrons, and positrons, for energies up to 50 MeV, and for alpha particles up

723

to 10 MeV; and in Tables A.4.1.1b, A.4.1.2b, A.4.1.3b, and Figures A.4.1.1b, A.4.1.2b, A.4.1.3b for724

photons from air kerma. The conversion coefficients relate the particle fluence to the value of the725

absorbed dose in local skin calculated for exposure of the specific phantoms for broad parallel beams

726

incident in specific directions, and a rotational field. Conversion coefficients are calculated as

727

follows:- for exposure of the trunk at the center of the front surface of a 300 mm x 300 mm x 150728

mm slab phantom of ICRU 4-element tissue density 1.0 g cm-3, for the volume of a right circular729

cylinder between depths of 50 and 100 µm and a cross sectional area of 1 cm² for angles, α, from 0°730(A-P) to 75° in 15° steps; for exposure of the extremity at the center of the cylindrical surface of a 73

731

mm diameter 300 mm length pillar phantom of ICRU 4-element tissue of density 1.11 g cm-³, for the732volume between the radii 36.4 mm and 36.45 with a circle of area 1 cm² projected onto the upper and733

lower cylindrical surfaces perpendicular to the radii, for angles, α, from 0° to 180° in 15° steps, and a734

rotational field; for exposure of the finger at the center of the cylindrical surface of a 19 mm diameter

735

300 mm length rod of ICRU 4-element tissue density 1.11 g cm-³, for the volume between the radii736

9.4 mm and 9.45 of a circle of area 1 cm² projected onto the upper and lower cylindrical surfaces

737

perpendicular to the radii, for angles, α, from 0° to 180° in 15° steps and a rotational field. Inside the738phantoms there is an outer layer of 2 mm skin of elemental composition given in ICRP Publication739

89 (2002) and of density of 1.09 g cm-3 (ICRP, 2009). The conversion coefficients for alpha particles

740

given in Table A.4.5 and Figure A.4.5 have been calculated for the volume of a right circular cylinder

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

741

between depths of 50 and 100 µm and a cross sectional area of 1 cm² at the center of the front surface742

of a 100 mm x 100 mm x 100 mm phantom of ICRU 4-element tissue density 1 g cm-³, without the743

2 mm skin layer (ICRP, 2010).

744

FINAL DRAFT JULY 2017

745
746

NOT TO BE REFERENCED

Table A.4.1.1a Conversion coefficients from photon fluence to directional and personal absorbed dosein local skin on the slab phantom (Daures et al., 2017).
dlocal skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

747
748
749

0.01

0
7.20E+00

15
7.17E+0030
7.14E+00

45
7.04E+00

60
6.89E+0075
6.38E+00

0.015

3.22E+00

3.20E+00

3.19E+00

3.17E+00

3.14E+00

3.04E+00

0.02

1.85E+00

1.83E+00

1.81E+00

1.80E+00

1.79E+00

1.73E+00

0.03

9.35E-01

9.24E-01

9.18E-01

9.05E-01

8.89E-01

8.24E-01

0.04

6.36E-01

6.47E-01

6.30E-01

5.26E-01

6.00E-01

5.45E-01

0.05

5.43E-01

5.46E-01

5.23E-01

5.26E-01

4.81E-01

4.49E-01

0.06

5.10E-01

5.06E-01

4.91E-01

4.85E-01

4.51E-01

4.25E-01

0.07

5.20E-01

5.14E-01

5.04E-01

4.87E-01

4.74E-01

4.48E-01

0.08

5.50E-01

5.31E-01

5.39E-01

5.24E-01

4.99E-01

4.63E-01

0.1

6.17E-01

6.09E-01

6.16E-01

6.21E-01

5.81E-01

5.63E-01

0.15

9.21E-01

9.04E-01

9.27E-01

8.95E-01

8.88E-01

8.66E-01

0.2

1.20E+00

1.21E+00

1.24E+00

1.19E+00

1.23E+00

1.20E+00

0.3

1.28E+00

1.34E+00

1.41E+00

1.46E+00

1.62E+00

1.69E+00

0.4

1.23E+00

1.29E+00

1.34E+00

1.49E+00

1.75E+00

1.87E+00

0.5

1.13E+00

1.16E+00

1.27E+00

1.49E+00

1.80E+00

2.07E+00

0.6

1.08E+00

1.11E+00

1.24E+00

1.47E+00

1.82E+00

2.25E+00

0.662

1.03E+00

1.08E+00

1.25E+00

1.41E+00

1.82E+00

2.26E+00

0.8

9.46E-01

9.89E-01

1.12E+00

1.41E+00

1.81E+00

2.40E+00

1

8.52E-01

8.87E-01

1.03E+00

1.33E+00

1.82E+00

2.62E+00

1.25

7.35E-01

7.98E-01

9.72E-01

1.23E+00

1.77E+00

2.65E+00

1.5

6.59E-01

7.06E-01

9.05E-01

1.23E+00

1.80E+00

2.78E+00

2

5.74E-01

6.23E-01

7.74E-01

1.05E+00

1.74E+00

2.98E+00

3

4.46E-01

4.66E-01

6.48E-01

9.71E-01

1.71E+00

3.17E+00

5

3.34E-01

3.57E-01

4.85E-01

7.33E-01

1.59E+00

3.44E+00

10

2.88E-01

3.05E-01

3.77E-01

5.88E-01

1.23E+00

3.72E+00

15

2.67E-01

2.80E-01

3.33E-01

5.02E-01

1.14E+00

3.78E+00

20

2.59E-01

2.58E-01

3.00E-01

4.96E-01

1.12E+00

3.93E+0030

2.43E-01

2.38E-01

3.03E-01

4.16E-01

9.71E-01

4.14E+00

50

2.13E-01

2.01E-01

2.82E-01

3.86E-01

8.26E-01

3.78E+00

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

750
751
752
753
754
755
756
757
758
759
760
761
762
763
764
765
766
767
768
769
770
771
772

Figure A.4.1.1a Conversion coefficients from photon fluence to directional and personal absorbed
dose in local skin on the slab phantom (Daures et al., 2017).

FINAL DRAFT JULY 2017

773
774

NOT TO BE REFERENCED

Table A.4.1.1b Conversion coefficients from photon air kerma to directional and personal absorbed dosein local skin on the slab phantom (Daures et al., 2017).
dlocal skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

775
776
777

0.01

0
9.73E-0115
9.69E-0130
9.65E-0145
9.51E-0160
9.31E-0175
8.62E-01

0.015

1.03E+00

1.02E+00

1.02E+00

1.01E+00

1.00E+00

9.73E-01

0.02

1.10E+00

1.09E+00

1.07E+00

1.07E+00

1.06E+00

1.03E+00

0.03

1.30E+00

1.28E+00

1.27E+00

1.25E+00

1.23E+00

1.14E+00

0.04

1.48E+00

1.51E+00

1.47E+00

1.23E+00

1.40E+00

1.27E+00

0.05

1.68E+00

1.69E+00

1.62E+00

1.63E+00

1.49E+00

1.39E+00

0.06

1.77E+00

1.75E+00

1.70E+00

1.68E+00

1.56E+00

1.47E+00

0.07

1.81E+00

1.79E+00

1.75E+00

1.69E+00

1.65E+00

1.56E+00

0.08

1.79E+00

1.73E+00

1.76E+00

1.71E+00

1.63E+00

1.51E+00

0.1

1.66E+00

1.64E+00

1.66E+00

1.67E+00

1.56E+00

1.52E+00

0.15

1.54E+00

1.51E+00

1.55E+00

1.49E+00

1.48E+00

1.44E+00

0.2

1.40E+00

1.41E+00

1.45E+00

1.39E+00

1.44E+00

1.40E+00

0.3

9.26E-01

9.69E-01

1.02E+00

1.06E+00

1.17E+00

1.22E+00

0.4

6.50E-01

6.82E-01

7.08E-01

7.88E-01

9.25E-01

9.88E-01

0.5

4.75E-01

4.88E-01

5.34E-01

6.26E-01

7.57E-01

8.70E-01

0.6

3.80E-01

3.90E-01

4.36E-01

5.17E-01

6.40E-01

7.91E-01

0.662

3.31E-01

3.47E-01

4.02E-01

4.53E-01

5.85E-01

7.26E-01

0.8

2.56E-01

2.67E-01

3.03E-01

3.81E-01

4.89E-01

6.48E-01

1

1.90E-01

1.98E-01

2.30E-01

2.97E-01

4.06E-01

5.85E-01

1.25

1.38E-01

1.50E-01

1.82E-01

2.31E-01

3.32E-01

4.97E-01

1.5

1.07E-01

1.15E-01

1.47E-01

2.00E-01

2.93E-01

4.52E-012

7.60E-02

8.24E-02

1.02E-01

1.39E-01

2.30E-01

3.94E-01

3

4.47E-02

4.67E-02

6.49E-02

9.73E-02

1.71E-01

3.18E-01

5

2.36E-02

2.52E-02

3.42E-02

5.17E-02

1.12E-01

2.43E-0110

1.19E-02

1.26E-02

1.56E-02

2.44E-02

5.10E-02

1.54E-01

15

7.75E-03

8.13E-03

9.66E-03

1.46E-02

3.31E-02

1.10E-01

20

5.71E-03

5.69E-03

6.61E-03

1.09E-02

2.47E-02

8.66E-0230

3.54E-03

3.47E-03

4.42E-03

6.07E-03

1.42E-02

6.04E-0250

1.79E-03

1.69E-03

2.37E-03

3.24E-03

6.93E-03

3.17E-02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

778
779
780
781
782
783
784
785
786
787
788
789
790
791

Figure A.4.1.1b Conversion coefficients from photon air kerma to directional and personal
absorbed dose in local skin on the slab phantom (Daures et al., 2017).

FINAL DRAFT JULY 2017

792
793

NOT TO BE REFERENCED

Table A.4.1.2a. Conversion coefficients from photon fluence to personal absorbed dose in local skin on
the pillar phantom (1/2) (Otto, 2017).
dp local skin / (pGy cm2)for a radiation incidence at 
Ep / MeV

794
795

0.002

0
2.94E+00

15
2.59E+0030
1.67E+00

45
6.73E-0160
1.10E-0175
2.05E-0390
3.28E-05

0.003

2.08E+01

1.98E+01

1.69E+01

1.20E+01

0.004

2.62E+01

2.57E+01

2.38E+01

2.04E+01

5.71E+00

8.73E-01

2.53E-03

1.43E+01

5.20E+00

9.54E-02

0.005

2.27E+01

2.24E+01

2.16E+01

0.007

1.40E+01

1.40E+01

1.37E+01

1.99E+01

1.65E+01

9.14E+00

5.56E-01

1.33E+01

1.24E+01

9.81E+00

1.83E+00

0.01

7.20E+00

7.22E+00

0.015

3.22E+00

3.22E+00

7.17E+00

7.14E+00

6.94E+00

6.37E+00

2.44E+00

3.22E+00

3.20E+00

3.18E+00

3.08E+00

2.00E+00

0.02

1.85E+00

0.03

8.97E-01

1.84E+00

1.85E+00

1.83E+00

1.81E+00

1.77E+00

1.41E+00

9.00E-01

9.04E-01

8.90E-01

8.86E-01

8.68E-01

7.72E-01

0.05

4.64E-01

4.67E-01

4.55E-01

4.63E-01

4.54E-01

4.50E-01

4.23E-01

0.07

4.19E-01

4.20E-01

4.17E-01

4.13E-01

4.13E-01

4.10E-01

3.90E-01

0.1

5.11E-01

5.11E-01

5.14E-01

5.09E-01

5.11E-01

5.13E-01

4.93E-01

0.15

7.77E-01

7.79E-01

7.73E-01

7.73E-01

7.83E-01

7.95E-01

7.74E-01

0.2

1.03E+00

1.04E+00

1.05E+00

1.06E+00

1.08E+00

1.11E+00

1.07E+00

0.3

1.11E+00

1.13E+00

1.19E+00

1.28E+00

1.42E+00

1.54E+00

1.58E+00

0.5

9.41E-01

9.72E-01

1.09E+00

1.28E+00

1.57E+00

1.90E+00

2.17E+00

0.662

8.19E-01

8.59E-01

9.85E-01

1.23E+00

1.58E+00

2.04E+00

2.47E+00

0.7

8.05E-01

8.37E-01

9.75E-01

1.21E+00

1.60E+00

2.08E+00

2.54E+00

1

6.63E-01

7.08E-01

8.32E-01

1.09E+00

1.60E+00

2.26E+00

2.98E+00

1.25

5.74E-01

6.08E-01

7.57E-01

1.10E+00

1.60E+00

2.35E+00

3.29E+00

1.5

5.33E-01

5.72E-01

7.29E-01

9.77E-01

1.56E+00

2.45E+00

3.53E+00

2

4.40E-01

4.63E-01

6.05E-01

9.11E-01

1.49E+00

2.57E+00

3.99E+00

3

3.24E-01

3.56E-01

4.96E-01

7.63E-01

1.37E+00

2.62E+00

4.69E+00

5

2.51E-01

2.76E-01

3.65E-01

5.63E-01

1.08E+00

2.48E+00

5.52E+00

7

2.03E-01

2.33E-01

2.92E-01

4.67E-01

8.95E-01

2.17E+00

6.06E+00

10

2.06E-01

1.94E-01

2.27E-01

3.74E-01

7.47E-01

1.81E+00

5.91E+00

15

1.81E-01

1.85E-01

2.11E-01

3.03E-01

5.35E-01

1.37E+00

5.44E+00

20

1.53E-01

1.54E-01

1.90E-01

2.47E-01

4.55E-01

1.15E+00

5.07E+00

30

1.49E-01

1.48E-01

1.58E-01

2.24E-01

3.73E-01

9.26E-01

4.67E+00

50

1.11E-01

1.11E-01

1.45E-01

1.76E-01

3.04E-01

7.51E-01

4.37E+00

FINAL DRAFT JULY 2017

796
797

NOT TO BE REFERENCED

Table A.4.1.2a Conversion coefficients from photon fluence to personal absorbed dose in local skin on
the pillar phantom (2/2) (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

798
799

0.002

105
0.00E+00120
0.00E+00135
0.00E+00

150
0.00E+00

165
0.00E+00

180
0.00E+00

ROT
5.43E-01

0.003

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

5.48E+00

0.004

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

8.55E+00

0.005

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

8.45E+00

0.007

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

6.01E+00

0.01

4.14E-03

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.41E+00

0.015

1.94E-01

1.07E-02

8.54E-04

1.52E-04

8.87E-05

3.80E-05

1.64E+00

0.02

4.41E-01

1.15E-01

3.88E-02

1.63E-02

1.05E-02

8.05E-03

1.01E+00

0.03

4.62E-01

2.65E-01

1.68E-01

1.24E-01

9.98E-02

9.86E-02

5.70E-01

0.05

3.24E-01

2.31E-01

1.86E-01

1.59E-01

1.43E-01

1.34E-01

3.38E-01

0.07

3.07E-01

2.40E-01

1.98E-01

1.67E-01

1.51E-01

1.49E-01

3.18E-01

0.1

3.99E-01

3.16E-01

2.63E-01

2.26E-01

2.17E-01

2.10E-01

4.03E-01

0.15

6.35E-01

5.25E-01

4.42E-01

3.99E-01

3.65E-01

3.56E-01

6.34E-01

0.2

9.12E-01

7.57E-01

6.46E-01

5.86E-01

5.39E-01

5.28E-01

8.87E-01

0.3

1.42E+00

1.21E+00

1.08E+00

9.82E-01

9.45E-01

9.33E-01

1.23E+00

0.5

2.12E+00

1.98E+00

1.85E+00

1.74E+00

1.68E+00

1.65E+00

1.64E+00

0.662

2.55E+00

2.48E+00

2.36E+00

2.28E+00

2.22E+00

2.18E+00

1.88E+00

0.7

2.66E+00

2.57E+00

2.46E+00

2.38E+00

2.32E+00

2.32E+00

1.93E+00

1

3.34E+00

3.36E+00

3.28E+00

3.24E+00

3.18E+00

3.19E+00

2.32E+00

1.25

3.75E+00

3.95E+00

3.93E+00

3.91E+00

3.92E+00

3.88E+00

2.62E+00

1.5

4.22E+00

4.48E+00

4.50E+00

4.47E+00

4.43E+00

4.49E+00

2.87E+00

2

4.97E+00

5.47E+00

5.63E+00

5.60E+00

5.62E+00

5.69E+00

3.37E+00

3

6.38E+00

7.19E+00

7.62E+00

7.67E+00

7.62E+00

7.67E+00

4.23E+00

5

8.92E+00

1.04E+01

1.11E+01

1.13E+01

1.14E+01

1.14E+01

5.77E+00

7

1.07E+01

1.33E+01

1.43E+01

1.47E+01

1.49E+01

1.49E+01

7.14E+00

10

1.28E+01

1.71E+01

1.90E+01

1.97E+01

2.00E+01

2.02E+01

9.01E+00

15

1.44E+01

2.18E+01

2.61E+01

2.79E+01

2.84E+01

2.86E+01

1.18E+0120

1.50E+01

2.43E+01

3.06E+01

3.41E+01

3.57E+01

3.60E+01

1.38E+0130

1.58E+01

2.71E+01

3.58E+01

4.13E+01

4.44E+01

4.53E+01

1.61E+0150

1.70E+01

3.07E+01

4.16E+01

4.93E+01

5.37E+01

5.53E+01

1.88E+01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

800
801
802
803
804
805
806
807
808
809
810
811
812
813
814
815
816
817
818
819
820
821
822
823
824
825
826
827
828
829
830

Figure A.4.1.2a Conversion coefficients from photon fluence to personal absorbed dose in local
skin on the pillar phantom (Otto, 2017).

FINAL DRAFT JULY 2017

831
832

NOT TO BE REFERENCED

Table A.4.1.2b Conversion coefficients from photon air kerma to personal absorbed dose in local skin on
the pillar phantom (1/2) (Otto, 2017).
dp local skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

833
834

0.002

0
1.80E-02

15
1.58E-0230
1.02E-0245
4.11E-0360
6.70E-0475
1.25E-0590
2.00E-07

0.003

2.76E-01

2.64E-01

2.24E-01

1.59E-01

7.59E-02

1.16E-02

3.36E-05

0.004

5.50E-01

5.39E-01

5.01E-01

4.28E-01

3.01E-01

1.09E-01

2.00E-03

0.005

7.40E-01

7.31E-01

7.04E-01

6.48E-01

5.38E-01

2.98E-01

1.81E-02

0.007

9.04E-01

9.01E-01

8.87E-01

8.60E-01

8.02E-01

6.33E-01

1.18E-01

0.01

9.74E-01

9.75E-01

9.69E-01

9.65E-01

9.38E-01

8.61E-01

3.30E-01

0.015

1.03E+00

1.03E+00

1.03E+00

1.02E+00

1.02E+00

9.86E-01

6.39E-01

0.02

1.10E+00

1.09E+00

1.10E+00

1.09E+00

1.07E+00

1.05E+00

8.35E-01

0.03

1.24E+00

1.25E+00

1.25E+00

1.23E+00

1.23E+00

1.20E+00

1.07E+00

0.05

1.44E+00

1.45E+00

1.41E+00

1.43E+00

1.41E+00

1.39E+00

1.31E+00

0.07

1.46E+00

1.46E+00

1.45E+00

1.43E+00

1.44E+00

1.43E+00

1.35E+00

0.1

1.37E+00

1.38E+00

1.38E+00

1.37E+00

1.37E+00

1.38E+00

1.33E+00

0.15

1.30E+00

1.30E+00

1.29E+00

1.29E+00

1.31E+00

1.33E+00

1.29E+00

0.2

1.20E+00

1.22E+00

1.23E+00

1.24E+00

1.26E+00

1.29E+00

1.25E+00

0.3

8.01E-01

8.14E-01

8.62E-01

9.27E-01

1.02E+00

1.11E+00

1.14E+00

0.5

3.96E-01

4.08E-01

4.57E-01

5.38E-01

6.58E-01

7.97E-01

9.11E-01

0.662

2.63E-01

2.76E-01

3.16E-01

3.97E-01

5.06E-01

6.56E-01

7.94E-01

0.7

2.46E-01

2.55E-01

2.98E-01

3.71E-01

4.88E-01

6.36E-01

7.75E-01

1

1.48E-01

1.58E-01

1.86E-01

2.43E-01

3.57E-01

5.04E-01

6.65E-01

1.25

1.08E-01

1.14E-01

1.42E-01

2.06E-01

3.00E-01

4.41E-01

6.17E-01

1.5

8.68E-02

9.30E-02

1.19E-01

1.59E-01

2.54E-01

3.99E-01

5.74E-01

2

5.82E-02

6.13E-02

8.01E-02

1.21E-01

1.97E-01

3.40E-01

5.28E-01

3

3.25E-02

3.57E-02

4.97E-02

7.65E-02

1.38E-01

2.62E-01

4.70E-01

5

1.77E-02

1.94E-02

2.57E-02

3.97E-02

7.60E-02

1.75E-01

3.90E-01

7

1.11E-02

1.28E-02

1.61E-02

2.57E-02

4.92E-02

1.20E-01

3.33E-01

10

8.54E-03

8.05E-03

9.39E-03

1.55E-02

3.09E-02

7.50E-02

2.45E-01

15

5.25E-03

5.36E-03

6.13E-03

8.80E-03

1.55E-02

3.98E-02

1.58E-0120

3.37E-03

3.40E-03

4.20E-03

5.45E-03

1.00E-02

2.54E-02

1.12E-0130

2.17E-03

2.16E-03

2.31E-03

3.27E-03

5.44E-03

1.35E-02

6.81E-0250

9.33E-04

9.27E-04

1.22E-03

1.48E-03

2.55E-03

6.30E-03

3.67E-02

FINAL DRAFT JULY 2017

835
836

NOT TO BE REFERENCED

Table A.4.1.2b Conversion coefficients from photon air kerma to personal absorbed dose in local skin on
the pillar phantom (2/2) (Otto, 2017).
dp local skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

837
838
839
840
841
842

0.002

105
0.00E+00120
0.00E+00135
0.00E+00

150
0.00E+00

165
0.00E+00

180
0.00E+00

ROT
3.32E-03

0.003

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

7.27E-02

0.004

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

1.80E-01

0.005

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.76E-01

0.007

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.88E-01

0.01

5.60E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

4.61E-01

0.015

6.21E-02

3.41E-03

2.73E-04

4.87E-05

2.84E-05

1.22E-05

5.26E-01

0.02

2.62E-01

6.85E-02

2.31E-02

9.66E-03

6.24E-03

4.78E-03

5.97E-01

0.03

6.40E-01

3.67E-01

2.33E-01

1.72E-01

1.38E-01

1.37E-01

7.90E-01

0.05

1.00E+00

7.15E-01

5.75E-01

4.92E-01

4.44E-01

4.16E-01

1.05E+00

0.07

1.07E+00

8.36E-01

6.87E-01

5.79E-01

5.26E-01

5.19E-01

1.10E+00

0.1

1.07E+00

8.51E-01

7.08E-01

6.09E-01

5.85E-01

5.65E-01

1.08E+00

0.15

1.06E+00

8.75E-01

7.37E-01

6.65E-01

6.08E-01

5.93E-01

1.06E+00

0.2

1.07E+00

8.84E-01

7.54E-01

6.84E-01

6.29E-01

6.16E-01

1.04E+00

0.3

1.03E+00

8.76E-01

7.82E-01

7.10E-01

6.84E-01

6.75E-01

8.91E-01

0.5

8.92E-01

8.32E-01

7.77E-01

7.33E-01

7.06E-01

6.93E-01

6.88E-01

0.662

8.20E-01

7.95E-01

7.58E-01

7.34E-01

7.14E-01

7.02E-01

6.04E-01

0.7

8.13E-01

7.85E-01

7.52E-01

7.27E-01

7.10E-01

7.08E-01

5.91E-01

1

7.45E-01

7.50E-01

7.32E-01

7.23E-01

7.10E-01

7.12E-01

5.18E-01

1.25

7.03E-01

7.41E-01

7.37E-01

7.33E-01

7.35E-01

7.28E-01

4.91E-01

1.5

6.87E-01

7.28E-01

7.32E-01

7.27E-01

7.21E-01

7.31E-01

4.67E-01

2

6.58E-01

7.23E-01

7.45E-01

7.42E-01

7.44E-01

7.52E-01

4.45E-01

3

6.39E-01

7.21E-01

7.64E-01

7.69E-01

7.64E-01

7.69E-01

4.24E-01

5

6.29E-01

7.33E-01

7.80E-01

7.97E-01

8.03E-01

8.04E-01

4.07E-01

7

5.89E-01

7.33E-01

7.89E-01

8.08E-01

8.19E-01

8.21E-01

3.92E-0110

5.30E-01

7.10E-01

7.88E-01

8.18E-01

8.30E-01

8.37E-01

3.74E-01

15

4.19E-01

6.33E-01

7.57E-01

8.10E-01

8.25E-01

8.29E-01

3.41E-0120

3.31E-01

5.35E-01

6.75E-01

7.52E-01

7.87E-01

7.94E-01

3.03E-0130

2.31E-01

3.95E-01

5.22E-01

6.02E-01

6.47E-01

6.61E-01

2.35E-0150

1.43E-01

2.57E-01

3.49E-01

4.13E-01

4.51E-01

4.64E-01

1.58E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

843
844
845
846
847
848
849
850
851
852
853
854
855
856
857
858
859
860
861
862
863
864
865
866
867
868
869
870
871
872
873
874
875
876
877
878
879
880
881
882
883
884
885
886
887

Figure A.4.1.2b Conversion coefficients from photon air kerma to personal absorbed dose in local
skin on the pillar phantom (Otto, 2017).

FINAL DRAFT JULY 2017

888
889

NOT TO BE REFERENCED

Table A.4.1.3a Conversion coefficients from photon fluence to personal absorbed dose in local skin on
the rod phantom (1/2) (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

890
891
892

0.002

0
2.54E+00

15
2.28E+0030
1.63E+00

45
9.08E-0160
3.62E-0175
8.54E-0290
0.00E+00

0.003

1.97E+01

1.87E+01

1.58E+01

1.14E+01

6.66E+00

2.91E+00

7.39E-01

0.004

2.56E+01

2.49E+01

2.29E+01

1.90E+01

1.32E+01

7.36E+00

2.84E+00

0.005

2.24E+01

2.21E+01

2.10E+01

1.88E+01

1.45E+01

9.19E+00

4.35E+00

0.007

1.39E+01

1.38E+01

1.36E+01

1.30E+01

1.14E+01

8.19E+00

4.71E+00

0.01

7.22E+00

7.21E+00

7.17E+00

7.06E+00

6.68E+00

5.44E+00

3.65E+00

0.015

3.23E+00

3.22E+00

3.21E+00

3.18E+00

3.11E+00

2.83E+00

2.29E+00

0.02

1.80E+00

1.80E+00

1.80E+00

1.79E+00

1.77E+00

1.69E+00

1.50E+00

0.03

8.14E-01

8.14E-01

8.13E-01

8.09E-01

8.03E-01

7.84E-01

7.41E-01

0.05

3.83E-01

3.82E-01

3.81E-01

3.79E-01

3.77E-01

3.71E-01

3.58E-01

0.06

3.43E-01

3.43E-01

3.43E-01

3.42E-01

3.41E-01

3.37E-01

3.26E-01

0.07

3.44E-01

3.44E-01

3.44E-01

3.44E-01

3.43E-01

3.39E-01

3.29E-01

0.1

4.36E-01

4.36E-01

4.36E-01

4.36E-01

4.36E-01

4.33E-01

4.24E-01

0.15

6.93E-01

6.93E-01

6.94E-01

6.96E-01

6.97E-01

6.93E-01

6.79E-01

0.2

9.51E-01

9.53E-01

9.57E-01

9.64E-01

9.73E-01

9.74E-01

9.59E-01

0.3

1.02E+00

1.04E+00

1.10E+00

1.18E+00

1.28E+00

1.37E+00

1.42E+00

0.5

8.71E-01

9.05E-01

1.01E+00

1.19E+00

1.44E+00

1.70E+00

1.94E+00

0.662

7.67E-01

8.08E-01

9.36E-01

1.16E+00

1.48E+00

1.86E+00

2.22E+00

0.7

7.49E-01

7.90E-01

9.19E-01

1.15E+00

1.48E+00

1.88E+00

2.27E+00

1

6.19E-01

6.65E-01

8.10E-01

1.08E+00

1.51E+00

2.06E+00

2.65E+00

1.25

5.34E-01

5.79E-01

7.28E-01

1.02E+00

1.50E+00

2.16E+00

2.90E+00

1.5

4.72E-01

5.16E-01

6.63E-01

9.64E-01

1.48E+00

2.23E+00

3.09E+00

2

3.89E-01

4.28E-01

5.62E-01

8.55E-01

1.41E+00

2.29E+00

3.39E+00

3

2.92E-01

3.20E-01

4.27E-01

6.74E-01

1.21E+00

2.22E+00

3.65E+00

5

2.04E-01

2.23E-01

2.90E-01

4.56E-01

8.71E-01

1.82E+00

3.45E+00

10

1.33E-01

1.43E-01

1.79E-01

2.70E-01

5.29E-01

1.27E+00

2.75E+00

15

1.09E-01

1.17E-01

1.44E-01

2.13E-01

4.23E-01

1.10E+00

2.53E+00

20

9.85E-02

1.05E-01

1.28E-01

1.87E-01

3.73E-01

1.02E+00

2.45E+00

30

8.76E-02

9.32E-02

1.13E-01

1.62E-01

3.28E-01

9.65E-01

2.43E+00

50

8.12E-02

8.56E-02

1.02E-01

1.46E-01

3.00E-01

9.53E-01

2.51E+00

FINAL DRAFT JULY 2017

893
894

NOT TO BE REFERENCED

Table A.4.1.3a Conversion coefficients from photon fluence to personal absorbed dose in local skin on
the rod phantom (2/2) (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

895
896
897
898
899
900
901
902
903
904
905
906
907

0.002

105
0.00E+00120
0.00E+00135
0.00E+00

150
0.00E+00

165
0.00E+00

180
0.00E+00

ROT
5.45E-01

0.003

4.71E-02

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

5.51E+00

0.004

4.55E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

8.62E+00

0.005

1.08E+00

1.93E-02

0.00E+00

0.00E+00

0.00E+00

0.00E+00

8.52E+00

0.007

1.77E+00

1.70E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

6.13E+00

0.01

1.85E+00

5.05E-01

5.54E-02

0.00E+00

0.00E+00

0.00E+00

3.60E+00

0.015

1.61E+00

9.41E-01

4.97E-01

2.91E-01

2.06E-01

1.84E-01

1.93E+00

0.02

1.24E+00

9.50E-01

7.16E-01

5.72E-01

4.97E-01

4.73E-01

1.29E+00

0.03

6.77E-01

6.02E-01

5.34E-01

4.86E-01

4.58E-01

4.49E-01

6.79E-01

0.05

3.39E-01

3.16E-01

2.95E-01

2.79E-01

2.69E-01

2.66E-01

3.39E-01

0.06

3.09E-01

2.89E-01

2.72E-01

2.59E-01

2.51E-01

2.48E-01

3.09E-01

0.07

3.14E-01

2.96E-01

2.78E-01

2.65E-01

2.57E-01

2.55E-01

3.13E-01

0.1

4.08E-01

3.89E-01

3.70E-01

3.56E-01

3.47E-01

3.44E-01

4.05E-01

0.15

6.57E-01

6.30E-01

6.05E-01

5.85E-01

5.71E-01

5.66E-01

6.53E-01

0.2

9.33E-01

8.95E-01

8.61E-01

8.39E-01

8.27E-01

8.25E-01

9.19E-01

0.3

1.44E+00

1.43E+00

1.40E+00

1.37E+00

1.35E+00

1.34E+00

1.30E+00

0.5

2.11E+00

2.20E+00

2.24E+00

2.25E+00

2.24E+00

2.24E+00

1.73E+00

0.662

2.50E+00

2.69E+00

2.79E+00

2.83E+00

2.85E+00

2.85E+00

1.99E+00

0.7

2.59E+00

2.79E+00

2.91E+00

2.96E+00

2.98E+00

2.99E+00

2.05E+00

1

3.17E+00

3.54E+00

3.77E+00

3.89E+00

3.95E+00

3.97E+00

2.45E+00

1.25

3.57E+00

4.08E+00

4.39E+00

4.57E+00

4.65E+00

4.68E+00

2.73E+00

1.5

3.92E+00

4.56E+00

4.97E+00

5.19E+00

5.30E+00

5.33E+00

2.98E+00

2

4.50E+00

5.41E+00

6.00E+00

6.33E+00

6.49E+00

6.53E+00

3.43E+00

3

5.27E+00

6.71E+00

7.73E+00

8.31E+00

8.59E+00

8.67E+00

4.13E+00

5

5.60E+00

7.86E+00

9.76E+00

1.11E+01

1.18E+01

1.20E+01

4.94E+00

10

4.93E+00

7.50E+00

9.93E+00

1.18E+01

1.30E+01

1.34E+01

4.92E+00

15

4.72E+00

7.37E+00

9.92E+00

1.19E+01

1.32E+01

1.36E+01

4.88E+00

20

4.68E+00

7.41E+00

1.01E+01

1.22E+01

1.35E+01

1.40E+01

4.93E+00

30

4.76E+00

7.67E+00

1.05E+01

1.28E+01

1.43E+01

1.48E+01

5.13E+00

50

5.02E+00

8.20E+00

1.14E+01

1.39E+01

1.55E+01

1.61E+01

5.51E+00

FINAL DRAFT JULY 2017

908
909
910
911
912
913
914
915
916
917
918
919
920
921
922
923
924
925
926
927
928
929
930
931
932
933
934
935
936
937
938
939
940
941
942
943
944
945
946
947
948
949

NOT TO BE REFERENCED

Figure A.4.1.3a Conversion coefficients from photon fluence to personal absorbed dose in local
skin on the rod phantom (Otto, 2017).

FINAL DRAFT JULY 2017

950
951

NOT TO BE REFERENCED

Table A.4.1.3b Conversion coefficients from photon air kerma to personal absorbed dose in local skin on
the rod phantom (1/2) (Otto, 2017).
dp local skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

952
953

0.002

0
1.55E-0215
1.39E-0230
9.96E-0345
5.55E-0360
2.21E-0375
5.22E-0490
0.00E+00

0.003

2.62E-01

2.48E-01

2.10E-01

1.51E-01

8.84E-02

3.86E-02

9.81E-03

0.004

5.38E-01

5.23E-01

4.81E-01

3.99E-01

2.77E-01

1.55E-01

5.96E-02

0.005

7.31E-01

7.21E-01

6.85E-01

6.13E-01

4.73E-01

3.00E-01

1.42E-01

0.007

8.97E-01

8.90E-01

8.77E-01

8.39E-01

7.35E-01

5.28E-01

3.04E-01

0.01

9.76E-01

9.74E-01

9.69E-01

9.54E-01

9.03E-01

7.35E-01

4.93E-01

0.015

1.03E+00

1.03E+00

1.03E+00

1.02E+00

9.95E-01

9.06E-01

7.33E-01

0.02

1.07E+00

1.07E+00

1.07E+00

1.06E+00

1.05E+00

1.00E+00

8.91E-01

0.03

1.13E+00

1.13E+00

1.13E+00

1.12E+00

1.11E+00

1.09E+00

1.03E+00

0.05

1.19E+00

1.18E+00

1.18E+00

1.17E+00

1.17E+00

1.15E+00

1.11E+00

0.06

1.19E+00

1.19E+00

1.19E+00

1.18E+00

1.18E+00

1.17E+00

1.13E+00

0.07

1.20E+00

1.20E+00

1.20E+00

1.20E+00

1.19E+00

1.18E+00

1.14E+00

0.1

1.17E+00

1.17E+00

1.17E+00

1.17E+00

1.17E+00

1.17E+00

1.14E+00

0.15

1.16E+00

1.16E+00

1.16E+00

1.16E+00

1.16E+00

1.16E+00

1.13E+00

0.2

1.11E+00

1.11E+00

1.12E+00

1.13E+00

1.14E+00

1.14E+00

1.12E+00

0.3

7.38E-01

7.52E-01

7.95E-01

8.53E-01

9.26E-01

9.91E-01

1.03E+00

0.5

3.66E-01

3.80E-01

4.25E-01

5.00E-01

6.05E-01

7.15E-01

8.15E-01

0.662

2.46E-01

2.60E-01

3.01E-01

3.73E-01

4.76E-01

5.98E-01

7.13E-01

0.7

2.29E-01

2.41E-01

2.81E-01

3.51E-01

4.52E-01

5.74E-01

6.93E-01

1

1.05E-01

1.15E-01

1.48E-01

2.15E-01

3.30E-01

4.98E-01

6.90E-01

1.25

1.00E-01

1.09E-01

1.37E-01

1.91E-01

2.81E-01

4.05E-01

5.44E-01

1.5

1.01E-01

1.08E-01

1.32E-01

1.76E-01

2.46E-01

3.35E-01

4.31E-01

2

5.15E-02

5.66E-02

7.44E-02

1.13E-01

1.87E-01

3.03E-01

4.49E-01

3

2.93E-02

3.21E-02

4.28E-02

6.76E-02

1.21E-01

2.23E-01

3.66E-015

1.44E-02

1.57E-02

2.05E-02

3.22E-02

6.14E-02

1.28E-01

2.43E-01

10

5.51E-03

5.93E-03

7.42E-03

1.12E-02

2.19E-02

5.26E-02

1.14E-01

15

3.16E-03

3.40E-03

4.18E-03

6.18E-03

1.23E-02

3.19E-02

7.34E-02

20

2.17E-03

2.31E-03

2.82E-03

4.12E-03

8.22E-03

2.25E-02

5.40E-0230

1.28E-03

1.36E-03

1.65E-03

2.36E-03

4.78E-03

1.41E-02

3.54E-0250

6.81E-04

7.18E-04

8.56E-04

1.22E-03

2.52E-03

7.99E-03

2.11E-02

FINAL DRAFT JULY 2017

954
955
956

Table A.4.1.3b Conversion coefficients from photon air kerma to personal absorbed dose in local skin on
the rod phantom (2/2) (Otto, 2017).
dp local skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

957
958
959

NOT TO BE REFERENCED

0.002

105
0.00E+00120
0.00E+00135
0.00E+00

150
0.00E+00

165
0.00E+00

180
0.00E+00

ROT
3.33E-03

0.003

6.25E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

7.32E-02

0.004

9.55E-03

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

1.81E-01

0.005

3.52E-02

6.30E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.78E-01

0.007

1.14E-01

1.10E-02

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.95E-01

0.01

2.50E-01

6.82E-02

7.49E-03

0.00E+00

0.00E+00

0.00E+00

4.86E-01

0.015

5.15E-01

3.01E-01

1.59E-01

9.31E-02

6.59E-02

5.89E-02

6.18E-01

0.02

7.36E-01

5.64E-01

4.25E-01

3.40E-01

2.95E-01

2.81E-01

7.66E-01

0.03

9.38E-01

8.34E-01

7.40E-01

6.73E-01

6.35E-01

6.22E-01

9.41E-01

0.05

1.05E+00

9.79E-01

9.14E-01

8.64E-01

8.33E-01

8.24E-01

1.05E+00

0.06

1.07E+00

1.00E+00

9.42E-01

8.97E-01

8.69E-01

8.58E-01

1.07E+00

0.07

1.09E+00

1.03E+00

9.66E-01

9.21E-01

8.93E-01

8.86E-01

1.09E+00

0.1

1.10E+00

1.05E+00

9.96E-01

9.59E-01

9.34E-01

9.26E-01

1.09E+00

0.15

1.10E+00

1.05E+00

1.01E+00

9.76E-01

9.53E-01

9.44E-01

1.09E+00

0.2

1.09E+00

1.04E+00

1.01E+00

9.79E-01

9.65E-01

9.63E-01

1.07E+00

0.3

1.04E+00

1.03E+00

1.01E+00

9.91E-01

9.76E-01

9.69E-01

9.40E-01

0.5

8.87E-01

9.25E-01

9.42E-01

9.46E-01

9.42E-01

9.42E-01

7.27E-01

0.662

8.03E-01

8.64E-01

8.97E-01

9.09E-01

9.16E-01

9.16E-01

6.39E-01

0.7

7.91E-01

8.52E-01

8.89E-01

9.04E-01

9.10E-01

9.13E-01

6.26E-011

8.75E-01

1.02E+00

1.11E+00

1.16E+00

1.18E+00

1.19E+00

6.65E-01

1.25

6.70E-01

7.65E-01

8.23E-01

8.57E-01

8.72E-01

8.78E-01

5.12E-01

1.5

5.16E-01

5.76E-01

6.13E-01

6.33E-01

6.43E-01

6.46E-01

3.99E-01

2

5.95E-01

7.16E-01

7.94E-01

8.38E-01

8.59E-01

8.64E-01

4.54E-01

3

5.28E-01

6.73E-01

7.75E-01

8.33E-01

8.61E-01

8.69E-01

4.14E-01

5

3.95E-01

5.54E-01

6.88E-01

7.83E-01

8.32E-01

8.46E-01

3.48E-01

10

2.04E-01

3.11E-01

4.12E-01

4.89E-01

5.39E-01

5.55E-01

2.04E-01

15

1.37E-01

2.14E-01

2.88E-01

3.45E-01

3.83E-01

3.95E-01

1.42E-0120

1.03E-01

1.63E-01

2.23E-01

2.69E-01

2.98E-01

3.09E-01

1.09E-0130

6.94E-02

1.12E-01

1.53E-01

1.87E-01

2.08E-01

2.16E-01

7.48E-0250

4.21E-02

6.88E-02

9.56E-02

1.17E-01

1.30E-01

1.35E-01

4.62E-02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

960
961
962
963
964
965
966
967
968
969
970
971
972
973
974
975
976
977
978
979
980
981
982
983
984
985
986
987
988
989
990
991
992
993
994
995
996
997
998
999
1000
1001
1002

Figure A.4.1.3b Conversion coefficients from photon air kerma to personal absorbed dose in local
skin on the rod phantom (Otto, 2017).

FINAL DRAFT JULY 2017

1003
1004

NOT TO BE REFERENCED

Table A.4.2.1 Conversion coefficients from neutron fluence to directional and personal absorbed dosein local skin on the slab phantom.

1005
1006
1007
1008
1009

Figure A.4.2.1 Conversion coefficients from neutron fluence to directional and personal absorbed dose in local
skin on the slab phantom.

FINAL DRAFT JULY 2017

1010
1011

NOT TO BE REFERENCED

Table A.4.2.2 Conversion coefficients from neutron fluence to personal absorbed dose in local skin on
the pillar phantom (1/2) (Hertel and Veinot, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV
1.00E-09
1.00E-08
2.50E-08
1.00E-07
2.00E-07
5.00E-07
1.00E-06
2.00E-06
5.00E-06
1.00E-05
2.00E-05
5.00E-05
1.00E-04
2.00E-04
5.00E-04
1.00E-03
2.00E-03
5.00E-03
1.00E-02
2.00E-02
3.00E-02
5.00E-02
7.00E-02
1.00E-01
1.50E-01
2.00E-01
3.00E-01
5.00E-01
7.00E-01
9.00E-01
1.00E+00
1.20E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
7.00E+00
8.00E+00
9.00E+00
1.00E+01
1.20E+01
1.40E+01
1.50E+01
1.60E+01
1.80E+01
2.00E+01

1012
1013

0
3.14E+00
1.77E+00
1.44E+00
1.18E+00
1.09E+00
9.87E-01
9.36E-01
8.41E-01
7.95E-01
7.34E-01
6.98E-01
6.31E-01
5.65E-01
5.35E-01
5.25E-01
5.50E-01
6.08E-01
8.93E-01
1.35E+00
2.23E+00
3.04E+00
4.46E+00
5.65E+00
7.18E+00
9.27E+00
1.10E+01
1.40E+01
1.74E+01
2.06E+01
2.41E+01
3.05E+01
2.77E+01
2.96E+01
3.29E+01
3.83E+01
4.45E+01
4.63E+01
5.10E+01
5.00E+01
5.27E+01
5.56E+01
5.82E+01
6.37E+01
6.59E+01
6.86E+01
6.87E+01
6.80E+01
6.99E+0115
3.10E+00
1.72E+00
1.43E+00
1.18E+00
1.08E+00
1.01E+00
9.21E-01
8.17E-01
7.97E-01
7.17E-01
6.84E-01
6.01E-01
5.44E-01
5.31E-01
5.37E-01
5.65E-01
6.05E-01
8.78E-01
1.34E+00
2.24E+00
3.03E+00
4.44E+00
5.65E+00
7.17E+00
9.28E+00
1.10E+01
1.40E+01
1.74E+01
2.06E+01
2.41E+01
3.05E+01
2.77E+01
2.96E+01
3.29E+01
3.83E+01
4.45E+01
4.63E+01
5.10E+01
4.99E+01
5.27E+01
5.53E+01
5.79E+01
6.33E+01
6.53E+01
6.78E+01
6.92E+01
6.78E+01
7.00E+0130
2.97E+00
1.67E+00
1.35E+00
1.10E+00
1.05E+00
9.43E-01
8.71E-01
8.26E-01
7.60E-01
7.44E-01
6.89E-01
6.06E-01
5.77E-01
5.38E-01
5.28E-01
5.53E-01
6.24E-01
8.97E-01
1.34E+00
2.25E+00
3.07E+00
4.47E+00
5.70E+00
7.23E+00
9.35E+00
1.11E+01
1.40E+01
1.76E+01
2.08E+01
2.43E+01
3.03E+01
2.78E+01
2.97E+01
3.31E+01
3.85E+01
4.47E+01
4.64E+01
5.10E+01
5.01E+01
5.29E+01
5.58E+01
5.83E+01
6.42E+01
6.62E+01
6.89E+01
6.97E+01
6.86E+01
7.12E+0145
2.83E+00
1.52E+00
1.24E+00
1.06E+00
9.80E-01
8.85E-01
8.59E-01
8.01E-01
7.33E-01
7.06E-01
6.39E-01
5.81E-01
5.68E-01
5.12E-01
5.14E-01
5.22E-01
6.20E-01
8.87E-01
1.37E+00
2.28E+00
3.10E+00
4.56E+00
5.80E+00
7.36E+00
9.49E+00
1.12E+01
1.42E+01
1.81E+01
2.12E+01
2.46E+01
3.02E+01
2.80E+01
3.00E+01
3.35E+01
3.88E+01
4.53E+01
4.66E+01
5.12E+01
5.06E+01
5.33E+01
5.59E+01
5.85E+01
6.45E+01
6.66E+01
6.94E+01
7.02E+01
6.95E+01
7.16E+0160
2.52E+00
1.34E+00
1.12E+00
9.44E-01
8.91E-01
8.62E-01
8.10E-01
7.45E-01
6.88E-01
6.69E-01
6.05E-01
5.70E-01
5.20E-01
4.93E-01
5.04E-01
5.14E-01
6.08E-01
9.02E-01
1.40E+00
2.33E+00
3.20E+00
4.67E+00
5.94E+00
7.56E+00
9.74E+00
1.15E+01
1.45E+01
1.87E+01
2.18E+01
2.52E+01
3.04E+01
2.85E+01
3.07E+01
3.42E+01
3.96E+01
4.63E+01
4.72E+01
5.18E+01
5.12E+01
5.41E+01
5.65E+01
5.91E+01
6.58E+01
6.75E+01
7.06E+01
7.09E+01
6.99E+01
7.22E+0175
2.02E+00
1.09E+00
9.15E-01
7.79E-01
7.72E-01
7.55E-01
6.95E-01
7.07E-01
6.43E-01
6.17E-01
5.67E-01
5.25E-01
4.88E-01
4.93E-01
4.75E-01
5.12E-01
5.90E-01
9.03E-01
1.39E+00
2.36E+00
3.22E+00
4.76E+00
6.05E+00
7.70E+00
9.94E+00
1.18E+01
1.48E+01
1.94E+01
2.24E+01
2.58E+01
3.07E+01
2.92E+01
3.16E+01
3.52E+01
4.07E+01
4.79E+01
4.83E+01
5.30E+01
5.22E+01
5.50E+01
5.77E+01
6.01E+01
6.67E+01
6.84E+01
7.13E+01
7.23E+01
7.13E+01
7.39E+0190
7.31E-01
5.65E-01
5.48E-01
5.71E-01
6.18E-01
6.14E-01
6.19E-01
5.98E-01
1.00E-20
5.22E-01
5.11E-01
4.97E-01
4.55E-01
4.50E-01
4.44E-01
4.42E-01
5.17E-01
7.14E-01
1.06E+00
1.78E+00
2.43E+00
3.65E+00
4.69E+00
6.09E+00
8.17E+00
9.92E+00
1.28E+01
1.75E+01
2.07E+01
2.39E+01
2.74E+01
2.75E+01
3.02E+01
3.39E+01
3.98E+01
4.72E+01
4.78E+01
1.00E-20
5.15E+01
5.45E+01
5.66E+01
5.86E+01
6.74E+01
6.64E+01
7.19E+01
7.18E+01
7.19E+01
7.29E+01

FINAL DRAFT JULY 2017

1014
1015

NOT TO BE REFERENCED

Table A.4.2 Conversion coefficients from neutron fluence to personal absorbed dose in local skin on thepillar phantom (2/2) (Hertel and Veinot, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV
1.00E-09
1.00E-08
2.50E-08
1.00E-07
2.00E-07
5.00E-07
1.00E-06
2.00E-06
5.00E-06
1.00E-05
2.00E-05
5.00E-05
1.00E-04
2.00E-04
5.00E-04
1.00E-03
2.00E-03
5.00E-03
1.00E-02
2.00E-02
3.00E-02
5.00E-02
7.00E-02
1.00E-01
1.50E-01
2.00E-01
3.00E-01
5.00E-01
7.00E-01
9.00E-01
1.00E+00
1.20E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
7.00E+00
8.00E+00
9.00E+00
1.00E+01
1.20E+01
1.40E+01
1.50E+01
1.60E+01
1.80E+01
2.00E+01

1016
1017

105
2.13E-01
2.47E-01
2.77E-01
3.75E-01
4.12E-01
4.77E-01
4.99E-01
4.98E-01
5.01E-01
4.88E-01
4.63E-01
4.28E-01
4.28E-01
4.07E-01
3.94E-01
3.69E-01
3.39E-01
3.81E-01
4.33E-01
5.80E-01
7.50E-01
1.11E+00
1.52E+00
2.12E+00
3.09E+00
4.09E+00
5.98E+00
9.36E+00
1.23E+01
1.51E+01
1.54E+01
1.84E+01
2.15E+01
2.59E+01
3.26E+01
3.90E+01
4.12E+01
4.53E+01
4.58E+01
4.81E+01
5.05E+01
5.19E+01
5.99E+01
6.14E+01
6.47E+01
6.60E+01
6.68E+01
7.00E+01120
1.78E-01
2.07E-01
2.39E-01
3.10E-01
3.55E-01
4.04E-01
4.28E-01
4.44E-01
4.44E-01
4.26E-01
4.27E-01
4.06E-01
3.92E-01
3.70E-01
3.53E-01
3.30E-01
3.22E-01
3.04E-01
3.11E-01
3.24E-01
3.61E-01
4.48E-01
5.59E-01
7.55E-01
1.22E+00
1.72E+00
2.79E+00
4.76E+00
7.15E+00
8.94E+00
8.13E+00
1.21E+01
1.54E+01
1.92E+01
2.48E+01
3.07E+01
3.37E+01
3.67E+01
3.93E+01
4.17E+01
4.35E+01
4.54E+01
4.88E+01
5.18E+01
5.42E+01
5.79E+01
5.56E+01
5.75E+01135
1.52E-01
1.87E-01
2.11E-01
2.86E-01
3.24E-01
3.79E-01
3.91E-01
3.94E-01
4.25E-01
4.18E-01
4.00E-01
3.91E-01
3.67E-01
3.50E-01
3.43E-01
3.15E-01
3.05E-01
2.95E-01
2.90E-01
2.71E-01
2.83E-01
3.00E-01
3.49E-01
4.33E-01
6.34E-01
9.21E-01
1.54E+00
2.93E+00
4.94E+00
6.42E+00
5.11E+00
9.05E+00
1.18E+01
1.58E+01
2.20E+01
2.72E+01
3.07E+01
3.29E+01
3.61E+01
3.89E+01
3.99E+01
4.18E+01
4.60E+01
4.78E+01
4.87E+01
5.50E+01
5.39E+01
5.65E+01150
1.45E-01
1.67E-01
1.91E-01
2.68E-01
2.93E-01
3.57E-01
3.76E-01
3.94E-01
3.99E-01
4.02E-01
3.94E-01
3.86E-01
3.63E-01
3.51E-01
3.20E-01
3.09E-01
3.00E-01
2.81E-01
2.77E-01
2.57E-01
2.43E-01
2.60E-01
2.80E-01
3.49E-01
4.51E-01
5.81E-01
1.05E+00
2.12E+00
3.62E+00
4.80E+00
3.90E+00
7.10E+00
9.56E+00
1.31E+01
1.93E+01
2.40E+01
2.80E+01
3.07E+01
3.39E+01
3.65E+01
3.81E+01
3.94E+01
4.27E+01
4.86E+01
4.92E+01
5.18E+01
5.10E+01
5.52E+01165
1.40E-01
1.72E-01
1.91E-01
2.54E-01
2.87E-01
3.45E-01
3.62E-01
3.77E-01
3.73E-01
3.78E-01
3.70E-01
3.47E-01
3.40E-01
3.30E-01
3.29E-01
2.98E-01
2.92E-01
2.64E-01
2.61E-01
2.62E-01
2.50E-01
2.54E-01
2.57E-01
2.90E-01
3.63E-01
4.90E-01
8.03E-01
1.71E+00
3.03E+00
4.12E+00
3.32E+00
6.05E+00
8.39E+00
1.21E+01
1.79E+01
2.24E+01
2.62E+01
2.90E+01
3.21E+01
3.43E+01
3.60E+01
3.82E+01
4.06E+01
4.67E+01
4.90E+01
5.06E+01
5.28E+01
5.55E+01180
1.42E-01
1.60E-01
1.80E-01
2.59E-01
2.82E-01
3.25E-01
3.53E-01
3.59E-01
3.72E-01
3.77E-01
3.55E-01
3.57E-01
3.43E-01
3.22E-01
3.25E-01
3.04E-01
2.86E-01
2.73E-01
2.69E-01
2.56E-01
2.33E-01
2.54E-01
2.59E-01
2.66E-01
3.41E-01
4.51E-01
7.54E-01
1.60E+00
2.91E+00
3.90E+00
3.11E+00
5.91E+00
8.16E+00
1.16E+01
1.76E+01
2.14E+01
2.54E+01
2.82E+01
3.22E+01
3.41E+01
3.57E+01
3.73E+01
4.14E+01
4.60E+01
4.81E+01
5.01E+01
5.26E+01
5.53E+01

ROT

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1018
1019
1020
1021
1022
1023
1024
1025
1026
1027
1028
1029
1030
1031
1032
1033
1034
1035
1036
1037
1038
1039
1040
1041

Figure A.4.2.2 Conversion coefficients from neutron fluence to personal absorbed dose in local skin on the pillar
phantom (Hertel and Veinot, 2017).

FINAL DRAFT JULY 2017

1042
1043

NOT TO BE REFERENCED

Table A.4.2.3 Conversion coefficients from neutron fluence to personal absorbed dose in local skin on the rod
phantom (1/2) (Hertel and Veinot, 2017).
dlocal skin / pGy cm2 for a radiation incidence at 
Ep / MeV
1.00E-09
1.00E-08
2.50E-08
1.00E-07
2.00E-07
5.00E-07
1.00E-06
2.00E-06
5.00E-06
1.00E-05
2.00E-05
5.00E-05
1.00E-04
2.00E-04
5.00E-04
1.00E-03
2.00E-03
5.00E-03
1.00E-02
2.00E-02
3.00E-02
5.00E-02
7.00E-02
1.00E-01
1.50E-01
2.00E-01
3.00E-01
5.00E-01
7.00E-01
9.00E-01
1.00E+00
1.20E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
7.00E+00
8.00E+00
9.00E+00
1.00E+01
1.20E+01
1.40E+01
1.50E+01
1.60E+01
1.80E+01
2.00E+01
3.00E+01
5.00E+011044

0
2.66E+00
1.22E+00
8.56E-01
4.95E-01
3.80E-01
2.55E-01
2.05E-01
1.44E-01
1.03E-01
8.05E-02
6.64E-02
5.28E-02
4.71E-02
5.03E-02
7.24E-02
1.22E-01
2.20E-01
5.21E-01
9.99E-01
1.89E+00
2.69E+00
4.11E+00
5.30E+00
6.77E+00
8.80E+00
1.06E+01
1.33E+01
1.66E+01
1.96E+01
2.26E+01
2.77E+01
2.59E+01
2.79E+01
3.12E+01
3.64E+01
4.23E+01
4.40E+01
4.79E+01
4.79E+01
5.08E+01
5.33E+01
5.56E+01
6.12E+01
6.36E+01
6.60E+01
6.70E+01
6.63E+01
6.86E+01
5.81E+01
5.25E+0115
2.64E+00
1.21E+00
8.59E-01
4.94E-01
3.76E-01
2.58E-01
2.03E-01
1.44E-01
1.01E-01
8.01E-02
6.67E-02
5.17E-02
4.78E-02
4.93E-02
7.25E-02
1.21E-01
2.22E-01
5.23E-01
1.00E+00
1.89E+00
2.70E+00
4.10E+00
5.28E+00
6.78E+00
8.81E+00
1.05E+01
1.32E+01
1.66E+01
1.96E+01
2.26E+01
2.77E+01
2.59E+01
2.79E+01
3.12E+01
3.65E+01
4.23E+01
4.40E+01
4.79E+01
4.79E+01
5.08E+01
5.33E+01
5.57E+01
6.13E+01
6.37E+01
6.60E+01
6.73E+01
6.66E+01
6.89E+01
5.83E+01
5.27E+0130
2.58E+00
1.18E+00
8.45E-01
4.85E-01
3.76E-01
2.61E-01
2.01E-01
1.46E-01
1.05E-01
8.09E-02
6.86E-02
5.36E-02
4.81E-02
5.02E-02
7.33E-02
1.22E-01
2.24E-01
5.26E-01
1.01E+00
1.90E+00
2.72E+00
4.12E+00
5.32E+00
6.82E+00
8.86E+00
1.05E+01
1.33E+01
1.67E+01
1.97E+01
2.27E+01
2.76E+01
2.60E+01
2.80E+01
3.13E+01
3.65E+01
4.24E+01
4.41E+01
4.79E+01
4.80E+01
5.08E+01
5.33E+01
5.56E+01
6.14E+01
6.37E+01
6.63E+01
6.75E+01
6.67E+01
6.89E+01
5.86E+01
5.34 E+0145
2.45E+00
1.13E+00
8.21E-01
4.79E-01
3.72E-01
2.58E-01
2.00E-01
1.49E-01
1.11E-01
8.59E-02
6.95E-02
5.47E-02
4.91E-02
5.03E-02
7.49E-02
1.23E-01
2.27E-01
5.33E-01
1.02E+00
1.93E+00
2.75E+00
4.17E+00
5.38E+00
6.90E+00
8.95E+00
1.06E+01
1.34E+01
1.69E+01
1.99E+01
2.29E+01
2.75E+01
2.61E+01
2.81E+01
3.14E+01
3.67E+01
4.26E+01
4.42E+01
4.80E+01
4.81E+01
5.09E+01
5.33E+01
5.56E+01
6.15E+01
6.38E+01
6.64E+01
6.79E+01
6.70E+01
6.91E+01
5.91 E+01
5.47 E+0160
2.12E+00
1.05E+00
7.51E-01
4.61E-01
3.68E-01
2.58E-01
2.04E-01
1.50E-01
1.16E-01
8.89E-02
7.06E-02
5.74E-02
4.95E-02
5.34E-02
6.85E-02
1.19E-01
2.23E-01
5.31E-01
1.02E+00
1.93E+00
2.76E+00
4.19E+00
5.42E+00
6.96E+00
9.06E+00
1.07E+01
1.34E+01
1.72E+01
2.01E+01
2.31E+01
2.74E+01
2.61E+01
2.81E+01
3.14E+01
3.68E+01
4.28E+01
4.42E+01
4.79E+01
4.78E+01
5.08E+01
5.34E+01
5.44E+01
5.82E+01
5.93E+01
6.13E+01
6.22E+01
6.24E+01
6.32E+01
6.21E+01
5.81E+0175
1.64E+00
8.68E-01
6.35E-01
4.24E-01
3.47E-01
2.50E-01
1.98E-01
1.46E-01
1.15E-01
8.81E-02
7.01E-02
5.68E-02
5.09E-02
5.16E-02
7.31E-02
1.16E-01
2.15E-01
5.11E-01
9.87E-01
1.87E+00
2.69E+00
4.10E+00
5.31E+00
6.85E+00
8.93E+00
1.07E+01
1.34E+01
1.73E+01
2.03E+01
2.32E+01
2.72E+01
2.63E+01
2.84E+01
3.18E+01
3.68E+01
4.28E+01
4.43E+01
4.78E+01
4.77E+01
5.10E+01
5.34E+01
5.44E+01
6.31E+01
6.60E+01
6.17E+01
6.32E+01
6.29E+01
6.40E+01
6.27E+01--90
1.07E+00
6.42E-01
5.25E-01
3.68E-01
3.12E-01
2.31E-01
1.85E-01
1.41E-01
1.11E-01
8.69E-02
6.99E-02
5.57E-02
4.94E-02
4.84E-02
6.12E-02
1.02E-01
1.88E-01
4.48E-01
8.69E-01
1.66E+00
2.39E+00
3.67E+00
4.79E+00
6.26E+00
8.25E+00
9.88E+00
1.25E+01
1.66E+01
1.95E+01
2.23E+01
2.57E+01
2.54E+01
2.77E+01
3.20E+01
3.65E+01
4.26E+01
4.41E+01
4.77E+01
4.78E+01
5.11E+01
5.34E+01
5.53E+01
6.30E+01
6.65E+01
6.63E+01
6.64E+01
6.57E+01
6.87E+01
6.04E+01
6.12E+01

FINAL DRAFT JULY 2017

1045
1046

NOT TO BE REFERENCED

Table A.4.2.3 Conversion coefficients from neutron fluence to personal absorbed dose in local skin on the rod
phantom (2/2) (Hertel and Veinot, 2017).
dlocal skin / pGy cm2 for a radiation incidence at 
Ep / MeV
1.00E-09
1.00E-08
2.50E-08
1.00E-07
2.00E-07
5.00E-07
1.00E-06
2.00E-06
5.00E-06
1.00E-05
2.00E-05
5.00E-05
1.00E-04
2.00E-04
5.00E-04
1.00E-03
2.00E-03
5.00E-03
1.00E-02
2.00E-02
3.00E-02
5.00E-02
7.00E-02
1.00E-01
1.50E-01
2.00E-01
3.00E-01
5.00E-01
7.00E-01
9.00E-01
1.00E+00
1.20E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
7.00E+00
8.00E+00
9.00E+00
1.00E+01
1.20E+01
1.40E+01
1.50E+01
1.60E+01
1.80E+01
2.00E+01
3.00E+01
5.00E+01

1047

105
6.44E-01
4.38E-01
3.78E-01
2.96E-01
2.65E-01
2.06E-01
1.71E-01
1.29E-01
1.06E-01
8.49E-02
6.78E-02
5.38E-02
4.65E-02
4.44E-02
5.79E-02
8.47E-02
1.54E-01
3.66E-01
7.10E-01
1.35E+00
1.98E+00
3.08E+00
4.09E+00
5.43E+00
7.16E+00
8.75E+00
1.13E+01
1.54E+01
1.82E+01
2.08E+01
2.34E+01
2.39E+01
2.63E+01
2.99E+01
3.53E+01
4.13E+01
4.30E+01
4.66E+01
4.69E+01
4.95E+01
5.17E+01
5.34E+01
6.31E+01
6.61E+01
6.74E+01
6.65E+01
6.62E+01
6.91E+01
6.04E+01
6.39E+01120
2.56E-01
2.64E-01
2.56E-01
2.35E-01
2.25E-01
1.83E-01
1.54E-01
1.24E-01
9.50E-02
8.00E-02
6.56E-02
4.96E-02
4.35E-02
4.00E-02
4.65E-02
6.78E-02
1.17E-01
2.64E-01
5.16E-01
1.00E+00
1.48E+00
2.39E+00
3.18E+00
4.33E+00
5.97E+00
7.35E+00
9.75E+00
1.37E+01
1.66E+01
1.90E+01
2.07E+01
2.20E+01
2.46E+01
2.84E+01
3.38E+01
3.94E+01
4.16E+01
4.47E+01
4.56E+01
4.81E+01
5.00E+01
5.17E+01
5.53E+01
5.70E+01
5.85E+01
6.01E+01
6.39E+01
6.80E+01
6.01E+01
6.52E+01135
1.51E-01
1.80E-01
1.91E-01
1.94E-01
1.94E-01
1.62E-01
1.36E-01
1.17E-01
9.12E-02
7.61E-02
6.24E-02
4.70E-02
3.95E-02
3.50E-02
3.66E-02
4.65E-02
8.00E-02
1.88E-01
3.66E-01
7.20E-01
1.08E+00
1.74E+00
2.42E+00
3.38E+00
4.81E+00
5.99E+00
8.26E+00
1.20E+01
1.48E+01
1.71E+01
1.80E+01
2.02E+01
2.31E+01
2.69E+01
3.21E+01
3.73E+01
4.00E+01
4.30E+01
4.45E+01
4.65E+01
4.82E+01
5.02E+01
5.35E+01
5.53E+01
5.73E+01
5.85E+01
5.92E+01
6.02E+01
5.90E+01
5.43E+01150
1.30E-01
1.58E-01
1.62E-01
1.76E-01
1.72E-01
1.51E-01
1.30E-01
1.08E-01
8.64E-02
7.32E-02
6.04E-02
4.56E-02
3.72E-02
3.33E-02
3.31E-02
3.61E-02
5.91E-02
1.38E-01
2.71E-01
5.45E-01
8.29E-01
1.39E+00
1.97E+00
2.78E+00
4.04E+00
5.18E+00
7.17E+00
1.07E+01
1.34E+01
1.56E+01
1.64E+01
1.93E+01
2.20E+01
2.58E+01
3.14E+01
3.68E+01
3.92E+01
4.22E+01
4.36E+01
4.61E+01
4.77E+01
4.96E+01
5.31E+01
5.50E+01
5.68E+01
5.82E+01
5.96E+01
6.51E+01
5.84E+01
5.35E+01165
1.30E-01
1.46E-01
1.53E-01
1.62E-01
1.66E-01
1.47E-01
1.27E-01
1.05E-01
8.57E-02
7.03E-02
5.85E-02
4.62E-02
3.74E-02
3.01E-02
3.00E-02
3.28E-02
5.16E-02
1.19E-01
2.35E-01
4.81E-01
7.33E-01
1.25E+00
1.80E+00
2.61E+00
3.84E+00
4.97E+00
7.03E+00
1.05E+01
1.33E+01
1.55E+01
1.57E+01
1.86E+01
2.16E+01
2.54E+01
3.12E+01
3.64E+01
3.91E+01
4.20E+01
4.36E+01
4.61E+01
4.78E+01
4.94E+01
5.28E+01
5.48E+01
5.67E+01
5.78E+01
5.95E+01
6.08E+01
5.81E+01
5.28E+01180
1.28E-01
1.46E-01
1.52E-01
1.58E-01
1.64E-01
1.44E-01
1.28E-01
1.03E-01
8.59E-02
7.00E-02
5.77E-02
4.60E-02
3.67E-02
3.14E-02
3.06E-02
3.19E-02
5.13E-02
1.15E-01
2.31E-01
4.67E-01
7.12E-01
1.24E+00
1.76E+00
2.58E+00
3.78E+00
4.89E+00
6.89E+00
1.04E+01
1.30E+01
1.53E+01
1.55E+01
1.85E+01
2.14E+01
2.53E+01
3.11E+01
3.63E+01
3.92E+01
4.18E+01
4.36E+01
4.60E+01
4.78E+01
4.94E+01
5.51E+01
5.33E+01
5.54E+01
5.64E+01
5.75E+01
5.85E+01
5.96E+01
6.78E+01

ROT

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1048
1049
1050
1051
1052
1053
1054
1055
1056
1057
1058
1059
1060
1061
1062
1063
1064
1065
1066
1067
1068
1069
1070
1071
1072

Figure A.4.2.3 Conversion coefficients from neutron fluence to personal absorbed dose in local skin on the rod
phantom (Hertel and Veinot, 2017)..

FINAL DRAFT JULY 2017

1073
1074

NOT TO BE REFERENCED

Table A.4.3.1 Conversion coefficients from electron fluence to directional and personal absorbed dose inlocal skin on the slab phantom (Daures et al., 2017).
dlocal skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1075
1076

0.01

0
1.18E-0315
1.24E-0330
1.25E-0345
9.98E-0460
5.93E-0475
2.30E-04

0.02

4.21E-03

4.27E-03

4.39E-03

2.92E-03

2.05E-03

9.30E-04

0.05

1.62E-02

1.97E-02

1.41E-02

1.25E-02

7.51E-03

3.77E-03

0.06

1.39E+01

1.16E+01

6.29E+00

2.13E+00

5.02E-01

8.94E-02

0.07

2.22E+02

1.92E+02

1.26E+02

6.01E+01

1.93E+01

3.52E+00

0.08

6.63E+02

5.94E+02

4.23E+02

2.31E+02

8.93E+01

2.00E+01

0.09

1.10E+03

1.00E+03

7.53E+02

4.45E+02

1.96E+02

5.05E+01

0.1

1.40E+03

1.30E+03

1.03E+03

6.53E+02

3.11E+02

8.91E+01

0.11

1.51E+03

1.42E+03

1.17E+03

7.91E+02

4.07E+02

1.25E+02

0.12

1.49E+03

1.42E+03

1.22E+03

8.67E+02

4.73E+02

1.56E+02

0.15

1.21E+03

1.20E+03

1.14E+03

9.22E+02

5.67E+02

2.05E+02

0.2

8.43E+02

8.73E+02

9.29E+02

8.67E+02

6.00E+02

2.34E+02

0.3

5.44E+02

5.67E+02

6.40E+02

7.23E+02

6.20E+02

2.64E+02

0.5

3.86E+02

3.98E+02

4.38E+02

5.15E+02

5.91E+02

3.20E+02

1

3.07E+02

3.12E+02

3.34E+02

3.70E+02

4.53E+02

4.31E+02

2

2.78E+02

2.82E+02

2.94E+02

3.19E+02

3.69E+02

4.74E+02

5

2.69E+02

2.69E+02

2.75E+02

2.89E+02

3.26E+02

3.96E+02

10

2.67E+02

2.70E+02

2.73E+02

2.80E+02

3.02E+02

3.61E+02

20

2.71E+02

2.71E+02

2.74E+02

2.78E+02

2.91E+02

3.39E+0230

2.72E+02

2.74E+02

2.76E+02

2.78E+02

2.86E+02

3.25E+0250

2.73E+02

2.75E+02

2.77E+02

2.78E+02

2.85E+02

3.11E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1077
1078
1079
1080
1081
1082
1083
1084
1085
1086
1087
1088
1089
1090
1091
1092
1093
1094
1095
1096
1097
1098
1099
1100
1101
1102

Figure A.4.3 Conversion coefficients from electron fluence to directional and personal absorbed
dose in local skin on the slab phantom (Daures et al., 2017).

FINAL DRAFT JULY 2017

1103
1104

NOT TO BE REFERENCED

Table A.4.3.2 Conversion coefficients from electron fluence to personal absorbed dose in local skin on
the pillar phantom (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV
0.05
0.055

0
2.61E-02
8.26E-0115
2.16E-02
6.68E-0130
1.70E-02
3.20E-0145
1.45E-02
1.09E-0160
8.24E-03
2.71E-0275
3.81E-03
5.52E-0390
0.00E+00
6.37E-04

0.06

2.26E+01

1.88E+01

1.08E+01

4.14E+00

0.065

1.13E+02

9.77E+01

6.19E+01

2.80E+01

1.04E+00

1.71E-01

8.45E-03

8.69E+00

1.68E+00

9.45E-02

0.07

2.77E+02

2.44E+02

1.65E+02

0.08

7.12E+02

6.43E+02

4.68E+02

8.30E+01

2.96E+01

6.62E+00

4.05E-01

2.66E+02

1.11E+02

3.00E+01

2.16E+00

0.09

1.14E+03

1.05E+03

0.1

1.39E+03

1.30E+03

8.00E+02

4.90E+02

2.27E+02

6.80E+01

5.30E+00

1.04E+03

6.81E+02

3.40E+02

1.11E+02

0.11

1.45E+03

9.33E+00

1.37E+03

1.14E+03

7.96E+02

4.26E+02

1.50E+02

1.33E+01

0.12
0.15

1.45E+03

1.37E+03

1.14E+03

7.96E+02

4.26E+02

1.49E+02

1.33E+01

1.13E+03

1.13E+03

1.07E+03

8.83E+02

5.62E+02

2.31E+02

2.29E+01

0.2

8.16E+02

8.35E+02

8.67E+02

8.16E+02

5.93E+02

2.67E+02

2.77E+01

0.3

5.46E+02

5.66E+02

6.28E+02

6.93E+02

6.03E+02

2.95E+02

3.11E+01

0.5

3.96E+02

4.07E+02

4.44E+02

5.16E+02

5.61E+02

3.37E+02

3.81E+01

1

3.13E+02

3.19E+02

3.38E+02

3.79E+02

4.58E+02

4.05E+02

5.83E+01

2

2.82E+02

2.85E+02

2.96E+02

3.21E+02

3.77E+02

4.53E+02

1.08E+02

5

2.71E+02

2.73E+02

2.76E+02

2.86E+02

3.14E+02

4.26E+02

2.93E+02

10

2.72E+02

2.72E+02

2.74E+02

2.78E+02

2.87E+02

3.28E+02

4.26E+02

20

2.72E+02

2.72E+02

2.74E+02

2.76E+02

2.81E+02

2.91E+02

3.40E+0250

2.72E+02

2.73E+02

2.74E+02

2.76E+02

2.79E+02

2.85E+02

3.00E+021105

dp local skin / (pGy cm2)for a radiation incidence at 
Ep / MeV

1106
1107

0.05
0.055

105
0.00E+00
0.00E+00120
0.00E+00
0.00E+00135
0.00E+00
0.00E+00

150
0.00E+00
0.00E+00

165
0.00E+00
0.00E+00

180
0.00E+00
0.00E+00

ROT
6.55E-03
1.29E-01

0.06

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.86E+00

0.065

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.12E+01

0.07

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

5.56E+01

0.08

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

1.56E+02

0.09

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.67E+02

0.1

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.48E+02

0.11

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.85E+02

0.12

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.85E+02

0.15

1.42E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.72E+02

0.2

2.26E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.18E+02

0.3

3.61E-04

3.91E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.57E+02

0.5

2.10E-03

6.68E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.08E+02

1

6.74E-03

5.01E-03

7.26E-03

0.00E+00

1.59E-03

1.31E-03

1.76E+02

2

2.80E-01

2.31E-02

2.88E-02

0.00E+00

2.96E-02

1.40E-02

1.65E+02

5

2.80E+01

1.32E+00

2.32E-01

2.80E-01

2.50E-01

2.10E-01

1.70E+02

10

2.17E+02

8.40E+01

1.85E+01

2.60E+00

1.02E+00

1.10E+00

1.94E+02

20

3.21E+02

3.11E+02

2.87E+02

2.53E+02

2.24E+02

2.12E+02

2.81E+02

50

3.06E+02

3.15E+02

3.23E+02

3.26E+02

3.27E+02

3.27E+02

2.99E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1108
1109
1110
1111
1112
1113
1114
1115
1116
1117
1118
1119
1120
1121
1122
1123
1124
1125
1126
1127
1128
1129
1130
1131
1132
1133
1134
1135
1136
1137
1138
1139
1140
1141
1142
1143
1144
1145
1146
1147
1148
1149
1150
1151
1152
1153
1154
1155

Figure A.4.3.2 Conversion coefficients from electron fluence to personal absorbed dose in local
skin on the pillar phantom (Otto, 2017).

FINAL DRAFT JULY 2017

1156
1157

Table A.4.3.3 Conversion coefficients from electron fluence to personal absorbed dose in local skin on
the rod phantom (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 

Ep / MeV
0.05
0.055

0
2.34E-02
6.44E-0115
2.20E-02
5.66E-0130
1.86E-02
3.79E-0145
1.41E-02
1.89E-0160
0.00E+00
6.86E-02

0.06

1.80E+01

1.60E+01

1.11E+01

5.93E+00

2.34E+00

6.59E-01

1.25E-01

0.065

9.10E+01

8.18E+01

5.92E+01

3.40E+01

1.51E+01

4.92E+00

1.09E+00

0.07

2.28E+02

2.07E+02

1.54E+02

9.34E+01

4.46E+01

1.61E+01

4.02E+00

0.08

6.22E+02

5.73E+02

4.45E+02

2.87E+02

1.51E+02

6.12E+01

1.76E+01

0.09

1.03E+03

9.61E+02

7.66E+02

5.18E+02

2.87E+02

1.25E+02

3.91E+01

0.1

1.28E+03

1.20E+03

9.86E+02

6.93E+02

4.05E+02

1.87E+02

6.20E+01

0.11

1.36E+03

1.28E+03

1.08E+03

7.88E+02

4.82E+02

2.34E+02

8.20E+01

0.12

1.33E+03

1.27E+03

1.09E+03

8.25E+02

5.23E+02

2.64E+02

9.63E+01

0.15

1.12E+03

1.10E+03

1.00E+03

8.18E+02

5.63E+02

3.08E+02

1.22E+02

0.2

8.32E+02

8.35E+02

8.17E+02

7.27E+02

5.47E+02

3.26E+02

1.39E+02

0.3

5.65E+02

5.84E+02

6.18E+02

6.08E+02

5.03E+02

3.30E+02

1.54E+02

0.5

4.06E+02

4.19E+02

4.57E+02

4.88E+02

4.42E+02

3.22E+02

1.73E+02

1

3.16E+02

3.22E+02

3.45E+02

3.90E+02

3.95E+02

3.22E+02

2.07E+02

2

2.82E+02

2.85E+02

2.95E+02

3.28E+02

3.69E+02

3.47E+02

2.69E+02

5

2.71E+02

2.71E+02

2.74E+02

2.80E+02

3.04E+02

3.29E+02

3.39E+02

10

2.71E+02

2.72E+02

2.73E+02

2.76E+02

2.84E+02

2.94E+02

3.01E+02

20

2.72E+02

2.72E+02

2.73E+02

2.75E+02

2.80E+02

2.85E+02

2.91E+0250

2.73E+02

2.73E+02

2.74E+02

2.76E+02

2.79E+02

2.83E+02

2.88E+021158

75
0.00E+00
1.87E-0290
0.00E+00
0.00E+00

dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1159
1160

NOT TO BE REFERENCED

0.05
0.055

105
0.00E+00
0.00E+00120
0.00E+00
1.17E-04135
0.00E+00
0.00E+00

150
0.00E+00
0.00E+00

165
0.00E+00
0.00E+00

180
0.00E+00
0.00E+00

ROT
6.97E-03
1.29E-01

0.06

1.36E-02

2.51E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.77E+00

0.065

1.31E-01

1.40E-03

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.01E+01

0.07

5.45E-01

6.60E-03

0.00E+00

0.00E+00

0.00E+00

0.00E+00

5.28E+01

0.08

2.75E+00

3.96E-02

0.00E+00

0.00E+00

0.00E+00

0.00E+00

1.54E+02

0.09

6.76E+00

1.07E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.68E+02

0.1

1.13E+01

2.03E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.49E+02

0.11

1.58E+01

2.90E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.87E+02

0.12

1.95E+01

3.81E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.96E+02

0.15

2.66E+01

6.12E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.75E+02

0.2

3.24E+01

8.99E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.20E+02

0.3

3.81E+01

1.39E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.60E+02

0.5

4.98E+01

2.66E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.13E+02

1

8.13E+01

9.60E+00

1.56E-01

0.00E+00

0.00E+00

0.00E+00

1.86E+02

2

1.56E+02

4.83E+01

9.55E+00

1.16E+00

7.53E-02

3.14E-02

1.87E+02

5

3.30E+02

2.94E+02

2.53E+02

2.21E+02

1.99E+02

1.92E+02

2.77E+02

10

3.06E+02

3.06E+02

3.05E+02

3.04E+02

3.04E+02

3.03E+02

2.93E+02

20

2.97E+02

3.01E+02

3.05E+02

3.08E+02

3.10E+02

3.10E+02

2.91E+0250

2.94E+02

3.00E+02

3.06E+02

3.10E+02

3.13E+02

3.14E+02

2.91E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1161
1162
1163
1164
1165
1166
1167
1168
1169
1170
1171
1172
1173
1174
1175
1176
1177
1178
1179
1180
1181
1182
1183
1184
1185
1186
1187
1188
1189
1190
1191
1192
1193
1194
1195
1196
1197
1198
1199
1200
1201
1202
1203
1204
1205
1206
1207

Figure A.4.3.3 Conversion coefficients from electron fluence to personal absorbed dose in local
skin on the rod phantom (Otto, 2017).

FINAL DRAFT JULY 2017

1208
1209

NOT TO BE REFERENCED

Table A.4.4.1 Conversion coefficients from positron fluence to directional and personal absorbed dose inlocal skin on the slab phantom (Daures et al., 2017).
dlocal skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1210
1211

0.01

0
1.17E+0115
1.11E+0130
9.91E+00

45
7.59E+00

60
4.89E+0075
2.02E+00

0.02

1.17E+01

1.11E+01

9.90E+00

7.55E+00

4.85E+00

2.02E+00

0.05

1.20E+01

1.11E+01

9.94E+00

7.70E+00

5.25E+00

1.91E+00

0.06

2.60E+01

2.35E+01

1.59E+01

9.71E+00

5.29E+00

2.03E+00

0.07

2.34E+02

2.04E+02

1.36E+02

6.79E+01

2.40E+01

5.53E+00

0.08

6.75E+02

6.04E+02

4.34E+02

2.39E+02

9.43E+01

2.21E+01

0.09

1.11E+03

1.01E+03

7.63E+02

4.53E+02

2.00E+02

5.24E+01

0.1

1.41E+03

1.31E+03

1.04E+03

6.60E+02

3.16E+02

9.12E+01

0.11

1.52E+03

1.43E+03

1.18E+03

7.99E+02

4.12E+02

1.28E+02

0.12

1.50E+03

1.44E+03

1.23E+03

8.75E+02

4.79E+02

1.58E+02

0.15

1.23E+03

1.22E+03

1.15E+03

9.31E+02

5.72E+02

2.08E+02

0.2

8.54E+02

8.83E+02

9.38E+02

8.73E+02

6.04E+02

2.36E+02

0.3

5.55E+02

5.77E+02

6.51E+02

7.31E+02

6.24E+02

2.66E+02

0.5

3.96E+02

4.07E+02

4.46E+02

5.20E+02

5.97E+02

3.22E+02

1

3.15E+02

3.20E+02

3.42E+02

3.77E+02

4.58E+02

4.33E+02

2

2.85E+02

2.88E+02

3.00E+02

3.23E+02

3.73E+02

4.76E+02

5

2.73E+02

2.73E+02

2.80E+02

2.93E+02

3.29E+02

3.97E+02

10

2.71E+02

2.74E+02

2.74E+02

2.82E+02

3.05E+02

3.63E+02

20

2.72E+02

2.73E+02

2.75E+02

2.80E+02

2.92E+02

3.39E+0230

2.72E+02

2.75E+02

2.77E+02

2.78E+02

2.86E+02

3.27E+0250

2.73E+02

2.75E+02

2.76E+02

2.78E+02

2.86E+02

3.10E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1212
1213
1214
1215
1216
1217
1218
1219
1220
1221
1222
1223
1224
1225
1226
1227
1228
1229
1230
1231
1232
1233
1234
1235
1236
1237

Figure A.4.4.1 Conversion coefficients from positron fluence to directional and personal
absorbed dose in local skin on the slab phantom (Daures et al., 2017).

FINAL DRAFT JULY 2017

1238
1239

NOT TO BE REFERENCED

Table A.4.4.2 Conversion coefficients from positron fluence to personal absorbed dose in local skin on
the pillar phantom (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV
0.01

0
1.08E+0115
1.03E+0130
9.36E+0045
7.64E+0060
5.50E+0075
3.23E+0090
1.47E+00

0.02

1.07E+01

1.04E+01

9.39E+00

7.64E+00

5.46E+00

3.27E+00

1.45E+00

0.05

1.09E+01

1.05E+01

9.40E+00

7.49E+00

5.25E+00

2.97E+00

1.35E+00

0.07

2.61E+02

2.30E+02

1.56E+02

8.03E+01

3.06E+01

8.55E+00

1.69E+00

0.1

1.40E+03

1.30E+03

1.04E+03

6.73E+02

3.34E+02

1.09E+02

1.02E+01

0.11

1.47E+03

1.39E+03

1.16E+03

7.99E+02

4.25E+02

1.48E+02

1.41E+01

0.15

1.17E+03

1.16E+03

1.10E+03

9.02E+02

5.72E+02

2.34E+02

2.42E+01

0.2

8.32E+02

8.51E+02

8.82E+02

8.30E+02

6.02E+02

2.72E+02

2.92E+01

0.5

3.99E+02

4.09E+02

4.45E+02

5.14E+02

5.57E+02

3.36E+02

3.90E+01

1

3.14E+02

3.19E+02

3.38E+02

3.76E+02

4.52E+02

4.00E+02

5.86E+01

2

2.83E+02

2.86E+02

2.95E+02

3.18E+02

3.71E+02

4.47E+02

1.08E+02

5

2.73E+02

2.73E+02

2.77E+02

2.86E+02

3.11E+02

4.17E+02

2.90E+02

10

2.71E+02

2.72E+02

2.73E+02

2.77E+02

2.84E+02

3.22E+02

4.15E+02

20

2.72E+02

2.72E+02

2.73E+02

2.76E+02

2.80E+02

2.89E+02

3.33E+0250

2.71E+02

2.72E+02

2.73E+02

2.75E+02

2.79E+02

2.84E+02

2.96E+021240
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1241
1242
1243
1244
1245
1246
1247
1248

0.01

105
9.85E-01120
7.85E-01135
6.93E-01150
6.92E-01165
6.27E-01180
5.78E-01

ROT
3.92E+00

0.02

9.50E-01

7.70E-01

7.07E-01

5.99E-01

5.91E-01

6.13E-01

3.91E+00

0.05

9.58E-01

8.26E-01

6.85E-01

6.46E-01

5.73E-01

5.88E-01

3.87E+00

0.07

8.90E-01

7.53E-01

6.80E-01

6.18E-01

6.12E-01

5.52E-01

5.34E+01

0.1

9.12E-01

7.52E-01

6.72E-01

6.08E-01

5.78E-01

5.36E-01

3.47E+02

0.11

9.15E-01

6.94E-01

6.82E-01

5.76E-01

5.36E-01

5.48E-01

3.89E+02

0.15

9.04E-01

8.13E-01

6.46E-01

6.30E-01

5.64E-01

5.93E-01

3.81E+02

0.2

9.29E-01

7.22E-01

6.37E-01

5.74E-01

6.44E-01

5.85E-01

3.24E+02

0.5

1.03E+00

7.81E-01

6.87E-01

6.15E-01

6.64E-01

7.07E-01

2.09E+02

1

1.08E+00

8.44E-01

7.50E-01

7.04E-01

6.56E-01

5.82E-01

1.75E+02

2

1.44E+00

1.16E+00

9.03E-01

7.50E-01

8.34E-01

7.77E-01

1.64E+02

5

3.01E+01

2.93E+00

1.71E+00

1.64E+00

1.46E+00

1.43E+00

1.69E+02

10

2.13E+02

8.55E+01

2.19E+01

5.30E+00

3.54E+00

3.39E+00

1.92E+02

20

3.06E+02

2.91E+02

2.69E+02

2.40E+02

2.15E+02

2.05E+02

2.73E+0250

2.99E+02

3.03E+02

3.05E+02

3.06E+02

3.05E+02

3.05E+02

2.90E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1249
1250
1251
1252
1253
1254
1255
1256
1257
1258
1259
1260
1261
1262
1263
1264
1265
1266
1267
1268
1269
1270
1271
1272
1273
1274
1275
1276
1277
1278
1279
1280
1281
1282
1283
1284
1285
1286
1287
1288
1289
1290
1291
1292
1293
1294

Figure A.4.4.2 Conversion coefficients from positron fluence to personal absorbed dose in local
skin on the pillar phantom (Otto, 2017).

FINAL DRAFT JULY 2017

1295
1296

NOT TO BE REFERENCED

Table A.4.4.3 Conversion coefficients from positron fluence to personal absorbed dose in local skin on
the rod phantom (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV
0.01

0
8.34E+00

15
8.08E+0030
7.33E+00

45
6.17E+00

60
4.77E+0075
3.38E+0090
2.29E+00

0.02

8.47E+00

8.19E+00

7.43E+00

6.23E+00

4.77E+00

3.35E+00

2.24E+00

0.05

8.61E+00

8.30E+00

7.44E+00

6.15E+00

4.62E+00

3.20E+00

2.13E+00

0.07

2.25E+02

2.04E+02

1.53E+02

9.35E+01

4.59E+01

1.79E+01

5.77E+00

0.1

1.28E+03

1.20E+03

9.82E+02

6.87E+02

4.00E+02

1.84E+02

6.16E+01

0.11

1.38E+03

1.30E+03

1.09E+03

7.93E+02

4.82E+02

2.33E+02

8.19E+01

0.15

1.15E+03

1.12E+03

1.02E+03

8.34E+02

5.73E+02

3.13E+02

1.24E+02

0.2

8.48E+02

8.51E+02

8.32E+02

7.40E+02

5.56E+02

3.31E+02

1.42E+02

0.5

4.04E+02

4.16E+02

4.52E+02

4.84E+02

4.41E+02

3.23E+02

1.76E+02

1

3.15E+02

3.21E+02

3.42E+02

3.85E+02

3.91E+02

3.21E+02

2.08E+02

2

2.81E+02

2.84E+02

2.93E+02

3.23E+02

3.64E+02

3.43E+02

2.69E+02

5

2.70E+02

2.71E+02

2.73E+02

2.79E+02

3.00E+02

3.21E+02

3.30E+02

10

2.71E+02

2.71E+02

2.72E+02

2.75E+02

2.82E+02

2.90E+02

2.95E+02

20

2.72E+02

2.72E+02

2.73E+02

2.75E+02

2.79E+02

2.83E+02

2.88E+0250

2.72E+02

2.73E+02

2.74E+02

2.76E+02

2.79E+02

2.82E+02

2.86E+021297
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1298
1299
1300
1301
1302

0.01

105
1.58E+00120
1.22E+00

135
1.09E+00

150
1.01E+00

165
9.71E-01180
9.76E-01

ROT
3.55E+00

0.02

1.55E+00

1.22E+00

1.09E+00

9.96E-01

9.34E-01

9.28E-01

3.56E+00

0.05

1.48E+00

1.17E+00

1.05E+00

9.89E-01

9.58E-01

9.54E-01

3.52E+00

0.07

1.98E+00

1.17E+00

1.03E+00

9.49E-01

9.13E-01

9.04E-01

5.32E+01

0.1

1.22E+01

1.37E+00

1.06E+00

9.65E-01

9.02E-01

8.70E-01

3.48E+02

0.11

1.67E+01

1.46E+00

1.05E+00

9.63E-01

9.10E-01

8.98E-01

3.91E+02

0.15

2.79E+01

1.77E+00

1.03E+00

9.65E-01

9.26E-01

9.17E-01

3.83E+02

0.2

3.41E+01

2.09E+00

1.06E+00

1.01E+00

9.76E-01

9.66E-01

3.26E+02

0.5

5.23E+01

4.14E+00

1.14E+00

1.06E+00

1.04E+00

1.03E+00

2.13E+02

1

8.42E+01

1.15E+01

1.53E+00

1.25E+00

1.18E+00

1.14E+00

1.86E+02

2

1.59E+02

5.21E+01

1.21E+01

2.91E+00

1.56E+00

1.48E+00

1.87E+02

5

3.20E+02

2.87E+02

2.50E+02

2.20E+02

2.00E+02

1.93E+02

2.74E+02

10

2.97E+02

2.94E+02

2.90E+02

2.88E+02

2.86E+02

2.86E+02

2.85E+02

20

2.91E+02

2.93E+02

2.95E+02

2.96E+02

2.97E+02

2.97E+02

2.86E+0250

2.91E+02

2.96E+02

3.00E+02

3.03E+02

3.05E+02

3.06E+02

2.88E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1303
1304
1305
1306
1307
1308
1309
1310
1311
1312
1313
1314
1315
1316
1317
1318
1319
1320
1321
1322
1323
1324
1325
1326
1327
1328
1329
1330
1331
1332
1333
1334
1335
1336
1337
1338
1339
1340
1341
1342
1343
1344
1345
1346

Figure A.4.4.3 Conversion coefficients from positron fluence to personal absorbed dose in local
skin on the rod phantom (Otto, 2017).

FINAL DRAFT JULY 2017

1347
1348

NOT TO BE REFERENCED

Table A.4.5 Conversion coefficients from alpha particle fluence to directional and personal absorbed
dose in local skin on the slab phantom (ICRP, 2010).
Ep / MeV
6.5
6.8
7.0
7.5
8.0
8.5
9.0
9.5
10.0

dlocal skin / (pGy cm2) for normal incidence
1.11E+03
2.56E+04
4.20E+04
7.52E+04
1.03E+05
1.28E+05
1.50E+05
1.72E+05
1.80E+05

1349
1350
1351
1352
1353
1354
1355
1356
1357
1358
1359
1360
1361
1362
1363

Figure A.4.5 Conversion coefficients from alpha particle fluence to directional andpersonal absorbed dose in local skin on the slab phantom (ICRP, 2010).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1364

A.5 Operational Quantities for Photons for Energies up to 50 MeV Calculated with the1365

Kerma-Approximation Method.

1366

The calibration of area monitoring instruments and personal dosimeters to measure photons for

1367

ambient dose, personal dose, directional and personal absorbed dose in the lens of the eye and local

1368

skin, are performed routinely in air with sufficient material in front of the instrument to provide full

1369

charged-particle equilibrium. The calibration procedure is for photons and for the particles produced in1370

air and the other material, at the point of test.

1371

Table A.5.1a and Figure A.5.1a give values of conversion coefficients for this procedure from1372

photon fluence to ambient dose for photon energies up to 50 MeV using the kerma-approximation to1373

approximate charged-particle equilibrium, in Table A.5.1b and Figure A.5.1b from air kerma; Table

1374

A.5.2a and Figure A.5.2a from photon fluence to personal dose, and in Table A.5.2 b and Figure A.5.2b

1375

from air kerma; Table A.5.3a and Figure A.5.3a from photon fluence to directional and personal

1376

absorbed dose in the lens of the eye, and in Table A.5.3b and Figure A.5.3b from air kerma; Tables

1377

A.5.4.1a, A5.4.2a, A5.4.3a, and Figures A.5.4.1a, A5.4.2a, A5.4.3a from photon fluence to directional1378

and personal absorbed dose in local skin, and in Tables A.5.4.1b, A5.4.2b, A5.4.3b and Figures A.5.4.1b,

1379

A5.4.2b, A5.4.3b from air kerma;

1380

FINAL DRAFT JULY 2017

1381
1382

NOT TO BE REFERENCED

Table A.5.1a Conversion coefficients from photon fluence to ambient dose calculated using the
kerma-approximation method (Endo, 2017).
Ep / MeV
1.00E-02
1.50E-02
2.00E-02
3.00E-02
4.00E-02
5.00E-02
6.00E-02
7.00E-02
8.00E-02
1.00E-01
1.50E-01
2.00E-01
3.00E-01
4.00E-01
5.00E-01
6.00E-01
8.00E-01
1.00E+00
1.50E+00
2.00E+00
3.00E+00
4.00E+00
5.00E+00
6.00E+00
8.00E+00
1.00E+01
1.50E+01
2.00E+01
3.00E+01
4.00E+01
5.00E+01

1383
1384

h*Emax/ (pSv cm2)
6.75E-02
1.53E-01
2.22E-01
3.10E-01
3.45E-01
3.64E-01
3.85E-01
4.11E-01
4.43E-01
5.19E-01
7.48E-01
9.98E-01
1.50E+00
2.00E+00
2.46E+00
2.91E+00
3.73E+00
4.49E+00
6.13E+00
7.54E+00
9.98E+00
1.21E+01
1.42E+01
1.61E+01
1.99E+01
2.37E+01
3.33E+01
4.32E+01
6.41E+01
8.63E+01
1.09E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1385
1386
1387
1388
1389
1390
1391
1392
1393
1394
1395
1396
1397
1398
1399
1400
1401
1402
1403

Figure A.5.1a Conversion coefficients from photon fluence to ambient dose calculated using the
kerma-approximation method (Endo, 2017).

FINAL DRAFT JULY 2017

1404
1405

NOT TO BE REFERENCED

Table A.5.1b Conversion coefficients from photon air kerma to ambient dose calculated using the
kerma-approximation method (Endo, 2017).
Ep / MeV
1.0E-02
1.5E-022.0E-02
3.0E-02
4.0E-02
5.0E-02
6.0E-02
7.0E-028.0E-02
1.0E-01
1.5E-01
2.0E-01
3.0E-01
4.0E-01
5.0E-01
6.0E-01
8.0E-01
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01

1406
1407
1408

h*Emax/ (Sv Gy-1)
9.12E-03
4.89E-02
1.32E-01
4.30E-01
8.05E-01
1.13E+00
1.33E+00
1.43E+00
1.44E+00
1.40E+00
1.25E+00
1.16E+00
1.09E+00
1.06E+00
1.04E+00
1.02E+00
1.01E+00
1.00E+00
9.98E-01
9.97E-01
1.00E+00
1.00E+00
1.00E+00
9.97E-01
9.89E-01
9.82E-01
9.65E-01
9.52E-01
9.34E-01
9.25E-01
9.17E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1409
1410
1411
1412
1413
1414
1415
1416
1417
1418
1419
1420
1421
1422
1423
1424
1425

Figure A.5.1b Conversion coefficients from photon air kerma to ambient dose calculated using
the kerma-approximation method (Endo, 2017).

FINAL DRAFT JULY 2017

1426
1427

NOT TO BE REFERENCED

Table A.5.2a Conversion coefficient from photon fluence to personal dose calculated using the kermaapproximation method (Endo, 2017).
hp() / (pSv cm2)
Ep / MeV
1.0E-02
1.5E-022.0E-02
3.0E-02
4.0E-02
5.0E-02
6.0E-02
7.0E-028.0E-02
1.0E-01
1.5E-01
2.0E-01
3.0E-01
4.0E-01
5.0E-01
6.0E-01
8.0E-01
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01

1428
1429

0
6.75E-02
1.53E-01
2.22E-01
3.10E-01
3.45E-01
3.64E-01
3.85E-01
4.11E-01
4.43E-01
5.19E-01
7.48E-01
9.98E-01
1.50E+00
2.00E+00
2.46E+00
2.91E+00
3.73E+00
4.49E+00
6.13E+00
7.54E+00
9.98E+00
1.21E+01
1.42E+01
1.61E+01
1.99E+01
2.37E+01
3.33E+01
4.32E+01
6.41E+01
8.63E+01
1.09E+02

max(15) max(30) max(45) max(60) max(75) max(90)
6.76E-02
1.51E-01
2.17E-01
3.07E-01
3.42E-01
3.62E-01
3.85E-01
4.08E-01
4.40E-01
5.15E-01
7.44E-01
9.93E-01
1.50E+00
1.99E+00
2.46E+00
2.90E+00
3.73E+00
4.49E+00
6.12E+00
7.53E+00
9.97E+00
1.21E+01
1.41E+01
1.61E+01
1.99E+01
2.37E+01
3.32E+01
4.31E+01
6.40E+01
8.62E+01
1.09E+02

6.20E-02
1.40E-01
2.04E-01
2.92E-01
3.27E-01
3.44E-01
3.66E-01
3.90E-01
4.21E-01
4.92E-01
7.18E-01
9.61E-01
1.46E+00
1.94E+00
2.40E+00
2.84E+00
3.66E+00
4.42E+00
6.05E+00
7.46E+00
9.89E+00
1.20E+01
1.40E+01
1.60E+01
1.98E+01
2.35E+01
3.30E+01
4.29E+01
6.36E+01
8.57E+01
1.09E+02

5.33E-02
1.19E-01
1.83E-01
2.63E-01
2.96E-01
3.15E-01
3.34E-01
3.58E-01
3.88E-01
4.59E-01
6.71E-01
9.04E-01
1.38E+00
1.85E+00
2.30E+00
2.74E+00
3.54E+00
4.28E+00
5.89E+00
7.30E+00
9.71E+00
1.19E+01
1.38E+01
1.58E+01
1.95E+01
2.32E+01
3.26E+01
4.23E+01
6.28E+01
8.45E+01
1.07E+02

4.27E-02
9.36E-02
1.46E-01
2.20E-01
2.52E-01
2.72E-01
2.92E-01
3.15E-01
3.41E-01
4.05E-01
5.99E-01
8.18E-01
1.27E+00
1.71E+00
2.14E+00
2.56E+00
3.34E+00
4.07E+00
5.65E+00
7.04E+00
9.43E+00
1.15E+01
1.35E+01
1.54E+01
1.91E+01
2.27E+01
3.20E+01
4.15E+01
6.16E+01
8.29E+01
1.05E+02

3.11E-02
6.54E-02
1.01E-01
1.63E-01
1.98E-01
2.16E-01
2.34E-01
2.55E-01
2.77E-01
3.35E-01
5.03E-01
6.95E-01
1.10E+00
1.51E+00
1.90E+00
2.30E+00
3.04E+00
3.73E+00
5.28E+00
6.63E+00
9.00E+00
1.11E+01
1.30E+01
1.49E+01
1.85E+01
2.21E+01
3.11E+01
4.04E+01
5.99E+01
8.06E+01
1.02E+02

1.89E-02
4.03E-02
6.25E-02
1.05E-01
1.34E-01
1.55E-01
1.70E-01
1.88E-01
2.07E-01
2.51E-01
3.85E-01
5.41E-01
8.69E-01
1.21E+00
1.55E+00
1.90E+00
2.56E+00
3.18E+00
4.62E+00
5.90E+00
8.17E+00
1.02E+01
1.21E+01
1.39E+01
1.74E+01
2.09E+01
2.96E+01
3.85E+01
5.71E+01
7.68E+01
9.73E+01

180

ROT

ISO

SS-ISO

IS-ISO

1.80E-02
1.53E-02
2.65E-02
9.61E-02
1.62E-01
2.07E-01
2.40E-01
2.71E-01
3.01E-01
3.61E-01
5.39E-01
7.35E-01
1.15E+00
1.57E+00
1.98E+00
2.37E+00
3.12E+00
3.82E+00
5.38E+00
6.75E+00
9.10E+00
1.12E+01
1.31E+01
1.50E+01
1.86E+01
2.22E+01
3.12E+01
4.05E+01
6.00E+01
8.08E+01
1.02E+02

3.31E-02
6.57E-02
9.97E-02
1.58E-01
1.97E-01
2.22E-01
2.44E-01
2.67E-01
2.95E-01
3.50E-01
5.21E-01
7.15E-01
1.11E+00
1.51E+00
1.90E+00
2.29E+00
3.01E+00
3.70E+00
5.22E+00
6.57E+00
8.90E+00
1.10E+01
1.29E+01
1.47E+01
1.83E+01
2.19E+01
3.09E+01
4.02E+01
5.96E+01
8.02E+01
1.02E+02

2.90E-02
5.45E-02
8.04E-02
1.24E-01
1.57E-01
1.78E-01
1.97E-01
2.16E-01
2.37E-01
2.85E-01
4.31E-01
5.94E-01
9.34E-01
1.28E+00
1.64E+00
1.98E+00
2.63E+00
3.25E+00
4.68E+00
5.95E+00
8.18E+00
1.02E+01
1.20E+01
1.38E+01
1.73E+01
2.07E+01
2.93E+01
3.82E+01
5.66E+01
7.62E+01
9.64E+01

2.94E-02
5.63E-02
8.00E-02
1.27E-01
1.60E-01
1.82E-01
2.01E-01
2.21E-01
2.43E-01
2.94E-01
4.44E-01
6.07E-01
9.64E-01
1.32E+00
1.68E+00
2.02E+00
2.69E+00
3.33E+00
4.77E+00
6.05E+00
8.32E+00
1.03E+01
1.22E+01
1.40E+01
1.75E+01
2.10E+01
2.96E+01
3.85E+01
5.72E+01
7.70E+01
9.75E+01

2.76E-02
5.33E-02
7.73E-02
1.22E-01
1.51E-01
1.72E-01
1.91E-01
2.11E-01
2.28E-01
2.76E-01
4.17E-01
5.72E-01
9.06E-01
1.25E+00
1.58E+00
1.91E+00
2.57E+00
3.18E+00
4.58E+00
5.83E+00
8.03E+00
1.00E+01
1.19E+01
1.36E+01
1.71E+01
2.05E+01
2.90E+01
3.77E+01
5.60E+01
7.54E+01
9.55E+01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1430
1431
1432
1433
1434
1435
1436
1437
1438
1439
1440
1441
1442
1443
1444
1445
1446
1447
1448
1449
1450
1451
1452
1453
1454
1455
1456
1457
1458
1459

Figure A.5.2a Conversion coefficient from photon fluence to personal dose calculated using the kermaapproximation method (Endo, 2017).

FINAL DRAFT JULY 2017

1460
1461

NOT TO BE REFERENCED

Table A.5.2b Conversion coefficient from photon air kerma to personal dose calculated using the kermaapproximation method (Endo, 2017).
hp() / (Sv Gy-1)
Ep / MeV
1.0E-02
1.5E-022.0E-02
3.0E-02
4.0E-02
5.0E-02
6.0E-02
7.0E-028.0E-02
1.0E-01
1.5E-01
2.0E-01
3.0E-01
4.0E-01
5.0E-01
6.0E-01
8.0E-01
1.0E+00
1.5E+00
2.0E+00
3.0E+00
4.0E+00
5.0E+00
6.0E+00
8.0E+00
1.0E+01
1.5E+01
2.0E+01
3.0E+01
4.0E+01
5.0E+01

1462
1463
1464

0
9.12E-03
4.89E-02
1.32E-01
4.30E-01
8.05E-01
1.13E+00
1.33E+00
1.43E+00
1.44E+00
1.40E+00
1.25E+00
1.16E+00
1.09E+00
1.06E+00
1.04E+00
1.02E+00
1.01E+00
1.00E+00
9.98E-01
9.97E-01
1.00E+00
1.00E+00
1.00E+00
9.97E-01
9.89E-01
9.82E-01
9.65E-01
9.52E-01
9.34E-01
9.25E-01
9.17E-01

max(15) max(30) max(45) max(60) max(75) max(90)
9.13E-03
4.84E-02
1.29E-01
4.25E-01
7.99E-01
1.12E+00
1.33E+00
1.42E+00
1.43E+00
1.39E+00
1.24E+00
1.16E+00
1.08E+00
1.05E+00
1.03E+00
1.02E+00
1.01E+00
1.00E+00
9.96E-01
9.97E-01
9.99E-01
9.99E-01
9.97E-01
9.95E-01
9.88E-01
9.81E-01
9.64E-01
9.50E-01
9.33E-01
9.24E-01
9.16E-01

8.38E-03
4.48E-02
1.21E-01
4.04E-01
7.63E-01
1.07E+00
1.27E+00
1.35E+00
1.37E+00
1.32E+00
1.20E+00
1.12E+00
1.06E+00
1.03E+00
1.01E+00
9.99E-01
9.90E-01
9.87E-01
9.84E-01
9.88E-01
9.91E-01
9.92E-01
9.90E-01
9.88E-01
9.82E-01
9.75E-01
9.59E-01
9.45E-01
9.28E-01
9.18E-01
9.10E-01

7.20E-03
3.81E-02
1.09E-01
3.64E-01
6.90E-01
9.76E-01
1.16E+00
1.24E+00
1.26E+00
1.24E+00
1.12E+00
1.06E+00
1.00E+00
9.80E-01
9.68E-01
9.62E-01
9.56E-01
9.55E-01
9.58E-01
9.66E-01
9.73E-01
9.76E-01
9.77E-01
9.75E-01
9.69E-01
9.62E-01
9.47E-01
9.33E-01
9.16E-01
9.06E-01
8.98E-01

5.77E-03
2.99E-02
8.68E-02
3.05E-01
5.88E-01
8.42E-01
1.01E+00
1.09E+00
1.11E+00
1.09E+00
9.99E-01
9.55E-01
9.18E-01
9.06E-01
9.00E-01
8.99E-01
9.01E-01
9.08E-01
9.19E-01
9.32E-01
9.45E-01
9.50E-01
9.53E-01
9.52E-01
9.47E-01
9.41E-01
9.28E-01
9.15E-01
8.98E-01
8.88E-01
8.81E-01

4.20E-03
2.09E-02
6.01E-02
2.26E-01
4.61E-01
6.68E-01
8.10E-01
8.85E-01
9.04E-01
9.02E-01
8.39E-01
8.11E-01
7.95E-01
7.97E-01
8.00E-01
8.07E-01
8.22E-01
8.32E-01
8.59E-01
8.78E-01
9.02E-01
9.12E-01
9.17E-01
9.19E-01
9.18E-01
9.15E-01
9.03E-01
8.91E-01
8.74E-01
8.64E-01
8.56E-01

2.55E-03
1.29E-02
3.71E-02
1.45E-01
3.12E-01
4.81E-01
5.89E-01
6.52E-01
6.76E-01
6.75E-01
6.43E-01
6.31E-01
6.28E-01
6.40E-01
6.53E-01
6.67E-01
6.90E-01
7.09E-01
7.52E-01
7.81E-01
8.19E-01
8.41E-01
8.53E-01
8.61E-01
8.65E-01
8.66E-01
8.59E-01
8.49E-01
8.33E-01
8.24E-01
8.16E-01

180

ROT

ISO

SS-ISO

IS-ISO

2.44E-03
4.90E-03
1.57E-02
1.33E-01
3.79E-01
6.40E-01
8.30E-01
9.41E-01
9.83E-01
9.71E-01
8.99E-01
8.58E-01
8.34E-01
8.29E-01
8.32E-01
8.35E-01
8.44E-01
8.52E-01
8.76E-01
8.93E-01
9.12E-01
9.20E-01
9.24E-01
9.26E-01
9.24E-01
9.19E-01
9.06E-01
8.93E-01
8.75E-01
8.66E-01
8.58E-01

4.47E-03
2.10E-02
5.92E-02
2.19E-01
4.60E-01
6.87E-01
8.44E-01
9.28E-01
9.62E-01
9.42E-01
8.69E-01
8.34E-01
8.06E-01
7.99E-01
8.01E-01
8.04E-01
8.13E-01
8.25E-01
8.50E-01
8.69E-01
8.92E-01
9.03E-01
9.08E-01
9.11E-01
9.10E-01
9.07E-01
8.96E-01
8.85E-01
8.69E-01
8.60E-01
8.52E-01

3.91E-03
1.74E-02
4.77E-02
1.72E-01
3.65E-01
5.52E-01
6.82E-01
7.49E-01
7.74E-01
7.67E-01
7.19E-01
6.93E-01
6.75E-01
6.79E-01
6.88E-01
6.95E-01
7.10E-01
7.25E-01
7.61E-01
7.87E-01
8.20E-01
8.39E-01
8.50E-01
8.56E-01
8.61E-01
8.59E-01
8.51E-01
8.41E-01
8.25E-01
8.16E-01
8.09E-01

3.98E-03
1.80E-02
4.75E-02
1.76E-01
3.74E-01
5.65E-01
6.96E-01
7.70E-01
7.93E-01
7.90E-01
7.41E-01
7.08E-01
6.97E-01
6.98E-01
7.04E-01
7.10E-01
7.25E-01
7.42E-01
7.76E-01
8.01E-01
8.34E-01
8.51E-01
8.61E-01
8.66E-01
8.70E-01
8.68E-01
8.60E-01
8.50E-01
8.34E-01
8.26E-01
8.18E-01

3.73E-03
1.71E-02
4.59E-02
1.69E-01
3.51E-01
5.33E-01
6.62E-01
7.32E-01
7.45E-01
7.44E-01
6.95E-01
6.68E-01
6.55E-01
6.59E-01
6.64E-01
6.72E-01
6.94E-01
7.10E-01
7.46E-01
7.71E-01
8.05E-01
8.25E-01
8.37E-01
8.43E-01
8.48E-01
8.48E-01
8.42E-01
8.32E-01
8.16E-01
8.09E-01
8.01E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1465
1466
1467
1468
1469
1470
1471
1472
1473
1474
1475
1476
1477
1478
1479
1480
1481
1482
1483
1484
1485
1486
1487
1488
1489
1490
1491
1492
1493

Figure A.5.2b Conversion coefficient from photon air kerma to personal dose calculated using the kermaapproximation method (Endo, 2017).

FINAL DRAFT JULY 2017

1494
1495
1496

NOT TO BE REFERENCED

Table A.5.3a Conversion coefficients from photons fluence to the maximum absorbed dose in thecomplete lens for left or right irradiations calculated using the kerma-approximation method (Behrens,
2017a).
dlens (α )/ (pGy cm2) for a radiation incidence at 

Ep / MeV
0.005
0.006
0.007
0.008
0.009
0.01
0.011
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.12
0.15
0.2
0.24
0.3
0.4
0.5
0.511
0.6
0.662
0.8
1
1.117
1.2
1.3
1.33
1.5
1.7
2
2.4
3
4
5
6
6.129
8
10
15
20
30
40
50

0

15

30

45

60

75

90

ROT

8.43E-06
2.01E-03
3.47E-02
1.73E-01
4.49E-01
7.96E-01
1.12E+00
1.54E+00
1.65E+00
1.58E+00
1.38E+00
1.11E+00
8.32E-01
5.87E-01
4.88E-01
4.55E-01
4.56E-01
4.81E-01
5.59E-01
6.64E-01
8.35E-01
1.13E+00
1.38E+00
1.74E+00
2.30E+00
2.82E+00
2.88E+00
3.33E+00
3.63E+00
4.24E+00
5.08E+00
5.54E+00
5.83E+00
6.20E+00
6.29E+00
6.88E+00
7.49E+00
8.39E+00
9.44E+00
1.10E+01
1.32E+01
1.53E+01
1.74E+01
1.76E+01
2.15E+01
2.54E+01
3.57E+01
4.63E+01
6.92E+01
9.30E+01
1.18E+02

1.56E-05
2.34E-03
3.55E-02
1.72E-01
4.40E-01
7.78E-01
1.10E+00
1.52E+00
1.63E+00
1.57E+00
1.38E+00
1.12E+00
8.36E-01
5.95E-01
4.90E-01
4.56E-01
4.62E-01
4.87E-01
5.62E-01
6.67E-01
8.39E-01
1.14E+00
1.39E+00
1.74E+00
2.34E+00
2.85E+00
2.90E+00
3.35E+00
3.65E+00
4.28E+00
5.10E+00
5.57E+00
5.91E+00
6.21E+00
6.31E+00
6.90E+00
7.53E+00
8.39E+00
9.49E+00
1.10E+01
1.32E+01
1.53E+01
1.74E+01
1.77E+01
2.14E+01
2.54E+01
3.58E+01
4.66E+01
6.91E+01
9.35E+01
1.19E+02

3.25E-05
2.97E-03
3.65E-02
1.64E-01
4.12E-01
7.30E-01
1.04E+00
1.46E+00
1.58E+00
1.54E+00
1.36E+00
1.11E+00
8.39E-01
5.96E-01
4.98E-01
4.64E-01
4.66E-01
4.91E-01
5.72E-01
6.73E-01
8.46E-01
1.15E+00
1.40E+00
1.76E+00
2.34E+00
2.88E+00
2.94E+00
3.39E+00
3.69E+00
4.30E+00
5.15E+00
5.63E+00
5.94E+00
6.27E+00
6.37E+00
6.92E+00
7.58E+00
8.44E+00
9.50E+00
1.10E+01
1.33E+01
1.54E+01
1.74E+01
1.77E+01
2.15E+01
2.55E+01
3.56E+01
4.65E+01
6.93E+01
9.33E+01
1.19E+02

3.23E-05
2.76E-03
3.19E-02
1.41E-01
3.56E-01
6.44E-01
9.34E-01
1.35E+00
1.50E+00
1.48E+00
1.32E+00
1.09E+00
8.32E-01
5.96E-01
4.99E-01
4.67E-01
4.67E-01
4.90E-01
5.71E-01
6.74E-01
8.50E-01
1.17E+00
1.41E+00
1.79E+00
2.37E+00
2.93E+00
2.99E+00
3.45E+00
3.77E+00
4.39E+00
5.25E+00
5.69E+00
5.99E+00
6.37E+00
6.46E+00
7.04E+00
7.67E+00
8.56E+00
9.63E+00
1.11E+01
1.33E+01
1.54E+01
1.75E+01
1.78E+01
2.15E+01
2.54E+01
3.56E+01
4.66E+01
6.91E+01
9.28E+01
1.18E+02

1.20E-05
1.46E-03
2.03E-02
9.78E-02
2.67E-01
5.08E-01
7.72E-01
1.19E+00
1.38E+00
1.39E+00
1.27E+00
1.06E+00
8.11E-01
5.90E-01
4.95E-01
4.62E-01
4.64E-01
4.88E-01
5.65E-01
6.72E-01
8.45E-01
1.15E+00
1.39E+00
1.75E+00
2.34E+00
2.90E+00
2.96E+00
3.42E+00
3.72E+00
4.38E+00
5.23E+00
5.68E+00
5.96E+00
6.36E+00
6.44E+00
7.05E+00
7.65E+00
8.53E+00
9.64E+00
1.11E+01
1.33E+01
1.55E+01
1.75E+01
1.78E+01
2.15E+01
2.54E+01
3.57E+01
4.64E+01
6.94E+01
9.32E+01
1.18E+02

1.59E-06
3.83E-04
7.95E-03
4.72E-02
1.51E-01
3.22E-01
5.36E-01
9.34E-01
1.16E+00
1.23E+00
1.17E+00
9.99E-01
7.78E-01
5.71E-01
4.79E-01
4.46E-01
4.52E-01
4.78E-01
5.59E-01
6.66E-01
8.39E-01
1.15E+00
1.38E+00
1.75E+00
2.32E+00
2.84E+00
2.90E+00
3.35E+00
3.65E+00
4.28E+00
5.13E+00
5.55E+00
5.89E+00
6.22E+00
6.34E+00
6.86E+00
7.49E+00
8.41E+00
9.48E+00
1.10E+01
1.32E+01
1.53E+01
1.74E+01
1.76E+01
2.14E+01
2.53E+01
3.55E+01
4.63E+01
6.91E+01
9.32E+01
1.18E+02

8.80E-08
4.32E-05
1.44E-03
1.35E-02
5.48E-02
1.39E-01
2.70E-01
5.79E-01
8.29E-01
9.58E-01
9.82E-01
8.87E-01
7.17E-01
5.35E-01
4.53E-01
4.27E-01
4.34E-01
4.60E-01
5.41E-01
6.44E-01
8.19E-01
1.13E+00
1.37E+00
1.73E+00
2.29E+00
2.85E+00
2.91E+00
3.36E+00
3.65E+00
4.29E+00
5.12E+00
5.56E+00
5.88E+00
6.25E+00
6.34E+00
6.90E+00
7.54E+00
8.37E+00
9.53E+00
1.09E+01
1.32E+01
1.53E+01
1.74E+01
1.76E+01
2.13E+01
2.54E+01
3.56E+01
4.62E+01
6.86E+01
9.23E+01
1.18E+02

6.67E-06
8.42E-04
1.15E-02
5.45E-02
1.44E-01
2.63E-01
3.87E-01
5.75E-01
6.60E-01
6.73E-01
6.28E-01
5.46E-01
4.41E-01
3.40E-01
2.98E-01
2.86E-01
2.95E-01
3.15E-01
3.77E-01
4.52E-01
5.81E-01
8.17E-01
1.00E+00
1.29E+00
1.75E+00
2.21E+00
2.25E+00
2.64E+00
2.91E+00
3.46E+00
4.21E+00
4.63E+00
4.92E+00
5.24E+00
5.36E+00
5.86E+00
6.48E+00
7.25E+00
8.33E+00
9.77E+00
1.19E+01
1.39E+01
1.59E+01
1.61E+01
1.94E+01
2.35E+01
3.28E+01
4.30E+01
6.39E+01
8.63E+01
1.09E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1497
1498
1499
1500
1501
1502
1503
1504
1505
1506
1507
1508
1509
1510
1511
1512
1513
1514
1515

Figure A.5.3a Conversion coefficients from photons fluence to the maximum absorbed dose in
the complete lens for left or right irradiations calculated using the kerma-approximation method(Behrens, 2017a).

FINAL DRAFT JULY 2017

1516
1517
1518

NOT TO BE REFERENCED

Table A.5.3b Conversion coefficients from photon air kerma to the maximum absorbed dose in thecomplete lens for left or right irradiations calculated using the kerma-approximation method (Behrens,
2017a).
dlens(α)/(Gy Gy-1) for a radiation incidence at 
Ep / MeV
0.005
0.006
0.007
0.008
0.009
0.01
0.011
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.12
0.15
0.2
0.24
0.3
0.4
0.5
0.511
0.6
0.662
0.8
1
1.117
1.2
1.3
1.33
1.5
1.7
2
2.4
3
4
5
6
6.129
8
10
15
20
30
40
50

0
2.75E-07
9.46E-05
2.24E-03
1.47E-02
4.87E-02
1.08E-01
1.86E-01
3.63E-01
5.27E-01
6.62E-01
8.20E-01
9.67E-01
1.15E+00
1.37E+00
1.51E+00
1.57E+00
1.58E+00
1.57E+00
1.51E+00
1.44E+00
1.39E+00
1.32E+00
1.30E+00
1.26E+00
1.22E+00
1.19E+00
1.19E+00
1.17E+00
1.17E+00
1.15E+00
1.13E+00
1.13E+00
1.13E+00
1.13E+00
1.12E+00
1.12E+00
1.11E+00
1.11E+00
1.10E+00
1.10E+00
1.09E+00
1.08E+00
1.07E+00
1.07E+00
1.07E+00
1.05E+00
1.04E+00
1.02E+00
1.01E+00
9.97E-01
9.92E-0115
5.10E-07
1.10E-04
2.29E-03
1.46E-02
4.77E-02
1.05E-01
1.83E-01
3.58E-01
5.21E-01
6.57E-01
8.17E-01
9.70E-01
1.16E+00
1.39E+00
1.52E+00
1.58E+00
1.61E+00
1.59E+00
1.51E+00
1.45E+00
1.40E+00
1.33E+00
1.31E+00
1.26E+00
1.23E+00
1.20E+00
1.19E+00
1.18E+00
1.17E+00
1.16E+00
1.14E+00
1.14E+00
1.14E+00
1.13E+00
1.13E+00
1.12E+00
1.12E+00
1.11E+00
1.11E+00
1.10E+00
1.09E+00
1.08E+00
1.08E+00
1.08E+00
1.06E+00
1.05E+00
1.04E+00
1.03E+00
1.01E+00
1.00E+00
9.99E-0130
1.06E-06
1.40E-04
2.36E-03
1.39E-02
4.47E-02
9.87E-02
1.73E-01
3.44E-01
5.06E-01
6.43E-01
8.05E-01
9.65E-01
1.16E+00
1.39E+00
1.54E+00
1.61E+00
1.62E+00
1.60E+00
1.54E+00
1.46E+00
1.41E+00
1.35E+00
1.31E+00
1.27E+00
1.24E+00
1.21E+00
1.21E+00
1.19E+00
1.19E+00
1.16E+00
1.15E+00
1.15E+00
1.15E+00
1.14E+00
1.14E+00
1.13E+00
1.13E+00
1.12E+00
1.11E+00
1.11E+00
1.10E+00
1.08E+00
1.08E+00
1.07E+00
1.07E+00
1.06E+00
1.03E+00
1.03E+00
1.01E+00
1.00E+00
9.96E-0145
1.05E-06
1.30E-04
2.06E-03
1.19E-02
3.86E-02
8.71E-02
1.55E-01
3.19E-01
4.81E-01
6.21E-01
7.84E-01
9.50E-01
1.15E+00
1.39E+00
1.54E+00
1.61E+00
1.62E+00
1.60E+00
1.54E+00
1.46E+00
1.42E+00
1.36E+00
1.33E+00
1.29E+00
1.25E+00
1.23E+00
1.23E+00
1.21E+00
1.21E+00
1.19E+00
1.17E+00
1.16E+00
1.16E+00
1.16E+00
1.15E+00
1.15E+00
1.14E+00
1.13E+00
1.12E+00
1.11E+00
1.10E+00
1.09E+00
1.08E+00
1.08E+00
1.07E+00
1.05E+00
1.03E+00
1.03E+00
1.01E+00
9.94E-01
9.93E-0160
3.92E-07
6.88E-05
1.31E-03
8.29E-03
2.89E-02
6.87E-02
1.28E-01
2.81E-01
4.41E-01
5.82E-01
7.54E-01
9.24E-01
1.12E+00
1.38E+00
1.53E+00
1.60E+00
1.61E+00
1.59E+00
1.52E+00
1.46E+00
1.41E+00
1.34E+00
1.31E+00
1.27E+00
1.24E+00
1.22E+00
1.22E+00
1.20E+00
1.20E+00
1.18E+00
1.17E+00
1.16E+00
1.15E+00
1.16E+00
1.15E+00
1.15E+00
1.14E+00
1.13E+00
1.13E+00
1.11E+00
1.10E+00
1.09E+00
1.08E+00
1.08E+00
1.07E+00
1.05E+00
1.04E+00
1.02E+00
1.01E+00
9.98E-01
9.88E-0175
5.20E-08
1.80E-05
5.13E-04
4.00E-03
1.64E-02
4.35E-02
8.87E-02
2.20E-01
3.72E-01
5.13E-01
6.92E-01
8.69E-01
1.08E+00
1.33E+00
1.48E+00
1.54E+00
1.57E+00
1.56E+00
1.50E+00
1.45E+00
1.40E+00
1.34E+00
1.30E+00
1.26E+00
1.23E+00
1.19E+00
1.19E+00
1.18E+00
1.17E+00
1.16E+00
1.14E+00
1.14E+00
1.14E+00
1.13E+00
1.13E+00
1.12E+00
1.11E+00
1.11E+00
1.11E+00
1.10E+00
1.08E+00
1.08E+00
1.07E+00
1.07E+00
1.06E+00
1.05E+00
1.03E+00
1.02E+00
1.01E+00
9.99E-01
9.91E-0190
2.87E-09
2.03E-06
9.28E-05
1.15E-03
5.95E-03
1.88E-02
4.47E-02
1.37E-01
2.65E-01
4.01E-01
5.83E-01
7.72E-01
9.94E-01
1.25E+00
1.40E+00
1.48E+00
1.51E+00
1.50E+00
1.46E+00
1.40E+00
1.37E+00
1.31E+00
1.29E+00
1.25E+00
1.21E+00
1.20E+00
1.20E+00
1.18E+00
1.17E+00
1.16E+00
1.14E+00
1.14E+00
1.14E+00
1.14E+00
1.13E+00
1.12E+00
1.12E+00
1.11E+00
1.11E+00
1.09E+00
1.08E+00
1.08E+00
1.08E+00
1.07E+00
1.06E+00
1.05E+00
1.03E+00
1.02E+00
1.00E+00
9.89E-01
9.88E-01

ROT
2.18E-07
3.96E-05
7.45E-04
4.62E-03
1.56E-02
3.56E-02
6.41E-02
1.36E-01
2.11E-01
2.82E-01
3.73E-01
4.75E-01
6.11E-01
7.92E-01
9.21E-01
9.89E-01
1.03E+00
1.03E+00
1.01E+00
9.82E-01
9.69E-01
9.54E-01
9.41E-01
9.34E-01
9.27E-01
9.29E-01
9.27E-01
9.29E-01
9.35E-01
9.35E-01
9.39E-01
9.47E-01
9.52E-01
9.53E-01
9.57E-01
9.54E-01
9.63E-01
9.60E-01
9.73E-01
9.79E-01
9.77E-01
9.80E-01
9.80E-01
9.79E-01
9.66E-01
9.73E-01
9.52E-01
9.48E-01
9.32E-01
9.26E-01
9.18E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1519
1520
1521
1522
1523
1524
1525
1526
1527
1528
1529
1530
1531
1532
1533
1534
1535
1536
1537
1538

Table A.5.3b Conversion coefficients from photons air kerma to the maximum absorbed dose in
the complete lens for left or right irradiations calculated using the kerma-approximation method(Behrens, 2017a).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1539
1540
1541

Table A.5.4.1a Conversion coefficient from photon fluence to directional and personal absorbed dose inlocal skin on the slab phantom, calculated using the kerma-approximation method (Daures et al., 2017).
dlocal skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1542
1543

0.01

0
7.16E+00

15
7.15E+0030
7.13E+00

45
7.04E+00

60
6.89E+0075
6.38E+00

0.015

3.20E+00

3.19E+00

3.19E+00

3.17E+00

3.14E+00

3.05E+00

0.02

1.84E+00

1.83E+00

1.83E+00

1.82E+00

1.80E+00

1.75E+00

0.03

9.28E-01

9.26E-01

9.21E-01

9.08E-01

8.83E-01

8.34E-01

0.04

6.47E-01

6.45E-01

6.40E-01

5.21E-01

6.01E-01

5.52E-01

0.05

5.43E-01

5.40E-01

5.35E-01

5.21E-01

4.97E-01

4.52E-01

0.06

5.10E-01

5.08E-01

5.02E-01

4.90E-01

4.67E-01

4.24E-01

0.07

5.15E-01

5.12E-01

5.07E-01

4.95E-01

4.72E-01

4.33E-01

0.08

5.40E-01

5.38E-01

5.33E-01

5.22E-01

5.01E-01

4.62E-01

0.1

6.25E-01

6.24E-01

6.21E-01

6.11E-01

5.92E-01

5.54E-01

0.15

9.14E-01

9.13E-01

9.15E-01

9.09E-01

8.97E-01

8.61E-01

0.2

1.23E+00

1.23E+00

1.23E+00

1.23E+00

1.23E+00

1.20E+00

0.3

1.84E+00

1.84E+00

1.86E+00

1.87E+00

1.89E+00

1.87E+00

0.4

2.42E+00

2.42E+00

2.44E+00

2.46E+00

2.50E+00

2.51E+00

0.5

2.96E+00

2.96E+00

2.99E+00

3.02E+00

3.07E+00

3.11E+00

0.6

3.47E+00

3.47E+00

3.50E+00

3.54E+00

3.61E+00

3.66E+00

0.662

3.77E+00

3.78E+00

3.81E+00

3.84E+00

3.92E+00

4.00E+00

0.8

4.40E+00

4.41E+00

4.44E+00

4.49E+00

4.58E+00

4.69E+00

1

5.24E+00

5.25E+00

5.29E+00

5.34E+00

5.45E+00

5.58E+00

1.25

6.18E+00

6.19E+00

6.23E+00

6.28E+00

6.40E+00

6.57E+00

1.5

7.03E+00

7.03E+00

7.08E+00

7.13E+00

7.26E+00

7.46E+00

2

8.55E+00

8.54E+00

8.59E+00

8.64E+00

8.79E+00

9.01E+00

3

1.11E+01

1.11E+01

1.12E+01

1.12E+01

1.13E+01

1.16E+01

5

1.55E+01

1.55E+01

1.56E+01

1.56E+01

1.57E+01

1.60E+01

10

2.57E+01

2.57E+01

2.57E+01

2.57E+01

2.58E+01

2.60E+01

15

3.60E+01

3.59E+01

3.60E+01

3.60E+01

3.61E+01

3.62E+01

20

4.67E+01

4.67E+01

4.68E+01

4.67E+01

4.69E+01

4.70E+0130

6.96E+01

6.95E+01

6.97E+01

6.96E+01

6.97E+01

6.97E+0150

1.19E+02

1.19E+02

1.19E+02

1.19E+02

1.19E+02

1.19E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1544
1545
1546
1547
1548
1549
1550
1551
1552
1553
1554
1555
1556
1557
1558
1559
1560
1561
1562
1563
1564
1565
1566
1567
1568
1569
1570
1571
1572
1573
1574
1575
1576
1577

Figure A.5.4.1a Conversion coefficient from photon fluence to directional and personal absorbed
dose in local skin on the slab phantom calculated using the kerma-approximation method(Daures et al., 2017).

FINAL DRAFT JULY 2017

1578
1579
1580

NOT TO BE REFERENCED

Table A.5.4.1b Conversion coefficient from photon air kerma to directional and personal absorbed dosein local skin on the slab phantom calculated using the kerma-approximation method (Daures et al.
2017).
dlocal skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

1581
1582
1583

0.01

0
9.68E-01

15
9.66E-0130
9.64E-0145
9.51E-0160
9.31E-0175
8.62E-01

0.015

1.02E+00

1.02E+00

1.02E+00

1.01E+00

1.00E+00

9.76E-01

0.02

1.09E+00

1.09E+00

1.09E+00

1.08E+00

1.07E+00

1.04E+00

0.03

1.29E+00

1.28E+00

1.28E+00

1.26E+00

1.22E+00

1.16E+00

0.04

1.51E+00

1.50E+00

1.49E+00

1.21E+00

1.40E+00

1.29E+00

0.05

1.68E+00

1.67E+00

1.66E+00

1.61E+00

1.54E+00

1.40E+00

0.06

1.77E+00

1.76E+00

1.74E+00

1.70E+00

1.62E+00

1.47E+00

0.07

1.79E+00

1.78E+00

1.76E+00

1.72E+00

1.64E+00

1.50E+00

0.08

1.76E+00

1.75E+00

1.74E+00

1.70E+00

1.63E+00

1.51E+00

0.1

1.68E+00

1.68E+00

1.67E+00

1.65E+00

1.59E+00

1.49E+00

0.15

1.52E+00

1.52E+00

1.53E+00

1.52E+00

1.50E+00

1.44E+00

0.2

1.44E+00

1.44E+00

1.44E+00

1.44E+00

1.44E+00

1.40E+00

0.3

1.33E+00

1.33E+00

1.34E+00

1.35E+00

1.37E+00

1.35E+00

0.4

1.28E+00

1.28E+00

1.29E+00

1.30E+00

1.32E+00

1.33E+00

0.5

1.24E+00

1.24E+00

1.26E+00

1.27E+00

1.29E+00

1.31E+00

0.6

1.22E+00

1.22E+00

1.23E+00

1.24E+00

1.27E+00

1.29E+00

0.662

1.21E+00

1.21E+00

1.22E+00

1.23E+00

1.26E+00

1.29E+00

0.8

1.19E+00

1.19E+00

1.20E+00

1.21E+00

1.24E+00

1.27E+00

1

1.17E+00

1.17E+00

1.18E+00

1.19E+00

1.22E+00

1.25E+00

1.25

1.16E+00

1.16E+00

1.17E+00

1.18E+00

1.20E+00

1.23E+00

1.5

1.14E+00

1.14E+00

1.15E+00

1.16E+00

1.18E+00

1.21E+00

2

1.13E+00

1.13E+00

1.14E+00

1.14E+00

1.16E+00

1.19E+00

3

1.11E+00

1.11E+00

1.12E+00

1.12E+00

1.13E+00

1.16E+00

5

1.09E+00

1.09E+00

1.10E+00

1.10E+00

1.11E+00

1.13E+00

10

1.07E+00

1.07E+00

1.07E+00

1.07E+00

1.07E+00

1.08E+00

15

1.04E+00

1.04E+00

1.04E+00

1.04E+00

1.05E+00

1.05E+00

20

1.03E+00

1.03E+00

1.03E+00

1.03E+00

1.03E+00

1.04E+00

30

1.01E+00

1.01E+00

1.02E+00

1.01E+00

1.02E+00

1.02E+00

50

9.98E-01

9.98E-01

9.98E-01

9.98E-01

9.98E-01

9.98E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1584
1585
1586
1587
1588
1589
1590
1591
1592
1593
1594
1595
1596
1597
1598
1599
1600
1601
1602
1603
1604
1605
1606
1607
1608
1609

Figure A.5.4.1b Conversion coefficient from photon air kerma to directional and personal
absorbed dose in local skin on the slab phantom calculated using the kerma-approximation
method (Daures et al., 2017).

FINAL DRAFT JULY 2017

1610
1611

NOT TO BE REFERENCED

Table A.5.4.2a Conversion coefficient from photon fluence to personal absorbed dose in local skin on
the pillar phantom calculated using the kerma-approximation method (1/2) (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1612
1613
1614
1615
1616
1617
1618
1619
1620
1621
1622

0.002

0
2.95E+00

15
2.58E+0030
1.67E+00

45
6.77E-0160
1.09E-0175
2.16E-0390
2.33E-05

0.003

2.08E+01

1.99E+01

1.69E+01

1.20E+01

0.004

2.62E+01

2.57E+01

2.39E+01

2.04E+01

5.71E+00

8.70E-01

2.59E-03

1.43E+01

5.19E+00

9.66E-02

0.005

2.26E+01

2.24E+01

2.16E+01

0.007

1.40E+01

1.39E+01

1.38E+01

1.98E+01

1.64E+01

9.14E+00

5.54E-01

1.34E+01

1.24E+01

9.83E+00

1.84E+00

0.01

7.23E+00

7.20E+00

0.015

3.22E+00

3.23E+00

7.20E+00

7.12E+00

6.93E+00

6.37E+00

2.44E+00

3.22E+00

3.19E+00

3.17E+00

3.09E+00

1.99E+00

0.02

1.84E+00

0.03

9.07E-01

1.85E+00

1.84E+00

1.84E+00

1.82E+00

1.78E+00

1.41E+00

9.04E-01

8.99E-01

8.93E-01

8.79E-01

8.67E-01

7.70E-01

0.05

4.64E-01

4.71E-01

4.59E-01

4.68E-01

4.59E-01

4.59E-01

4.28E-01

0.07

4.22E-01

4.18E-01

4.19E-01

4.12E-01

4.13E-01

4.13E-01

3.89E-01

0.1

5.19E-01

5.14E-01

5.18E-01

5.14E-01

5.07E-01

5.12E-01

4.89E-01

0.15

7.87E-01

7.87E-01

7.86E-01

7.89E-01

7.89E-01

7.95E-01

7.69E-01

0.2

1.08E+00

1.09E+00

1.09E+00

1.09E+00

1.09E+00

1.11E+00

1.07E+00

0.3

1.68E+00

1.67E+00

1.67E+00

1.68E+00

1.70E+00

1.72E+00

1.69E+00

0.5

2.78E+00

2.78E+00

2.77E+00

2.80E+00

2.82E+00

2.85E+00

2.85E+00

0.662

3.62E+00

3.57E+00

3.55E+00

3.61E+00

3.66E+00

3.65E+00

3.66E+00

0.7

3.77E+00

3.77E+00

3.75E+00

3.78E+00

3.85E+00

3.83E+00

3.85E+00

1

5.13E+00

5.03E+00

5.02E+00

5.06E+00

5.15E+00

5.21E+00

5.20E+00

1.25

6.00E+00

5.99E+00

5.97E+00

6.00E+00

6.07E+00

6.18E+00

6.14E+00

1.5

6.96E+00

6.86E+00

6.83E+00

6.92E+00

6.97E+00

6.98E+00

6.94E+00

2

8.38E+00

8.30E+00

8.31E+00

8.24E+00

8.36E+00

8.79E+00

8.34E+00

3

1.10E+01

1.11E+01

1.11E+01

1.09E+01

1.12E+01

1.12E+01

1.08E+01

5

1.58E+01

1.53E+01

1.51E+01

1.54E+01

1.56E+01

1.50E+01

1.55E+01

7

1.96E+01

1.94E+01

1.95E+01

1.96E+01

1.95E+01

1.93E+01

1.94E+01

10

2.56E+01

2.56E+01

2.58E+01

2.55E+01

2.51E+01

2.52E+01

2.54E+01

15

3.71E+01

3.55E+01

3.53E+01

3.65E+01

3.61E+01

3.65E+01

3.61E+01

20

4.85E+01

4.53E+01

4.67E+01

4.73E+01

4.64E+01

4.71E+01

4.71E+0130

7.16E+01

6.92E+01

6.95E+01

7.08E+01

6.98E+01

6.95E+01

6.91E+0150

1.20E+02

1.19E+02

1.19E+02

1.22E+02

1.20E+02

1.19E+02

1.20E+02

FINAL DRAFT JULY 2017

1623
1624

NOT TO BE REFERENCED

Table A.5.4.2a Conversion coefficient from photon fluence to personal absorbed dose in local skin on
the pillar phantom calculated using the kerma-approximation method (2/2) (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1625
1626
1627
1628
1629
1630

0.002

105
0.00E+00120
0.00E+00135
0.00E+00

150
0.00E+00

165
0.00E+00

180
0.00E+00

ROT
5.43E-01

0.003

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

5.48E+00

0.004

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

8.56E+00

0.005

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

8.44E+00

0.007

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

6.01E+00

0.01

4.60E-03

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.41E+00

0.015

1.94E-01

1.17E-02

8.12E-04

1.39E-04

2.81E-05

3.28E-05

1.64E+00

0.02

4.40E-01

1.17E-01

3.79E-02

1.71E-02

1.02E-02

7.85E-03

1.01E+00

0.03

4.61E-01

2.68E-01

1.67E-01

1.25E-01

1.02E-01

9.23E-02

5.70E-01

0.05

3.23E-01

2.35E-01

1.85E-01

1.49E-01

1.35E-01

1.41E-01

3.39E-01

0.07

3.11E-01

2.39E-01

1.96E-01

1.70E-01

1.52E-01

1.52E-01

3.18E-01

0.1

4.01E-01

3.20E-01

2.63E-01

2.35E-01

2.13E-01

2.12E-01

4.04E-01

0.15

6.47E-01

5.27E-01

4.51E-01

3.94E-01

3.67E-01

3.53E-01

6.39E-01

0.2

9.14E-01

7.48E-01

6.49E-01

5.83E-01

5.41E-01

5.37E-01

8.98E-01

0.3

1.46E+00

1.26E+00

1.12E+00

9.94E-01

9.48E-01

9.45E-01

1.43E+00

0.5

2.54E+00

2.23E+00

2.00E+00

1.88E+00

1.81E+00

1.74E+00

2.47E+00

0.662

3.33E+00

2.93E+00

2.68E+00

2.52E+00

2.45E+00

2.35E+00

3.22E+00

0.7

3.49E+00

3.11E+00

2.84E+00

2.67E+00

2.56E+00

2.51E+00

3.39E+00

1

4.72E+00

4.38E+00

3.93E+00

3.79E+00

3.74E+00

3.67E+00

4.64E+00

1.25

5.65E+00

5.29E+00

4.93E+00

4.71E+00

4.50E+00

4.45E+00

5.56E+00

1.5

6.53E+00

6.07E+00

5.71E+00

5.58E+00

5.36E+00

5.41E+00

6.41E+00

2

8.09E+00

7.43E+00

7.14E+00

6.83E+00

6.80E+00

6.66E+00

7.85E+00

3

1.07E+01

1.02E+01

9.51E+00

9.51E+00

9.05E+00

9.23E+00

1.04E+01

5

1.52E+01

1.46E+01

1.38E+01

1.34E+01

1.34E+01

1.34E+01

1.48E+01

7

1.87E+01

1.81E+01

1.74E+01

1.79E+01

1.70E+01

1.71E+01

1.87E+01

10

2.47E+01

2.44E+01

2.38E+01

2.28E+01

2.29E+01

2.27E+01

2.46E+01

15

3.49E+01

3.42E+01

3.32E+01

3.15E+01

3.27E+01

3.18E+01

3.48E+01

20

4.54E+01

4.47E+01

4.28E+01

4.26E+01

4.15E+01

4.19E+01

4.51E+0130

6.64E+01

6.49E+01

6.50E+01

6.40E+01

6.41E+01

6.14E+01

6.73E+0150

1.14E+02

1.12E+02

1.10E+02

1.06E+02

1.03E+02

1.03E+02

1.15E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1631
1632
1633
1634
1635
1636
1637
1638
1639
1640
1641
1642
1643
1644
1645
1646
1647
1648
1649
1650
1651
1652
1653
1654
1655
1656
1657
1658
1659
1660
1661
1662
1663
1664
1665
1666
1667
1668
1669
1670
1671
1672
1673
1674

Figure A.5.4.2a Conversion coefficient from photon fluence to personal absorbed dose in local
skin on the pillar phantom calculated using the kerma-approximation method (Otto, 2017).

FINAL DRAFT JULY 2017

1675
1676

NOT TO BE REFERENCED

Table A.5.4.2b Conversion coefficient from photon air kerma to personal absorbed dose in local skin on
the pillar phantom calculated using the kerma-approximation method (1/2) (Otto, 2017).
dp local skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

1677
1678
1679
1680
1681
1682
1683
1684
1685
1686
1687

0.002

0
1.80E-02

15
1.58E-0230
1.02E-0245
4.13E-0360
6.67E-0475
1.32E-0590
1.42E-07

0.003

2.77E-01

2.64E-01

2.25E-01

1.59E-01

7.58E-02

1.15E-02

3.44E-05

0.004

5.51E-01

5.39E-01

5.01E-01

4.28E-01

3.01E-01

1.09E-01

2.03E-03

0.005

7.39E-01

7.31E-01

7.04E-01

6.47E-01

5.37E-01

2.98E-01

1.81E-02

0.007

9.02E-01

8.99E-01

8.88E-01

8.61E-01

8.02E-01

6.34E-01

1.19E-01

0.01

9.76E-01

9.73E-01

9.73E-01

9.62E-01

9.37E-01

8.61E-01

3.30E-01

0.015

1.03E+00

1.03E+00

1.03E+00

1.02E+00

1.01E+00

9.90E-01

6.36E-01

0.02

1.09E+00

1.10E+00

1.09E+00

1.09E+00

1.08E+00

1.06E+00

8.37E-01

0.03

1.26E+00

1.25E+00

1.25E+00

1.24E+00

1.22E+00

1.20E+00

1.07E+00

0.05

1.44E+00

1.46E+00

1.42E+00

1.45E+00

1.42E+00

1.42E+00

1.32E+00

0.07

1.47E+00

1.45E+00

1.45E+00

1.43E+00

1.43E+00

1.44E+00

1.35E+00

0.1

1.40E+00

1.38E+00

1.40E+00

1.38E+00

1.37E+00

1.38E+00

1.32E+00

0.15

1.31E+00

1.31E+00

1.31E+00

1.32E+00

1.32E+00

1.33E+00

1.28E+00

0.2

1.26E+00

1.27E+00

1.27E+00

1.27E+00

1.27E+00

1.29E+00

1.25E+00

0.3

1.21E+00

1.21E+00

1.21E+00

1.21E+00

1.23E+00

1.24E+00

1.22E+00

0.5

1.17E+00

1.17E+00

1.16E+00

1.18E+00

1.19E+00

1.20E+00

1.20E+00

0.662

1.16E+00

1.15E+00

1.14E+00

1.16E+00

1.17E+00

1.17E+00

1.18E+00

0.7

1.15E+00

1.15E+00

1.15E+00

1.16E+00

1.18E+00

1.17E+00

1.18E+00

1

1.14E+00

1.12E+00

1.12E+00

1.13E+00

1.15E+00

1.16E+00

1.16E+00

1.25

1.13E+00

1.12E+00

1.12E+00

1.13E+00

1.14E+00

1.16E+00

1.15E+00

1.5

1.13E+00

1.12E+00

1.11E+00

1.13E+00

1.13E+00

1.14E+00

1.13E+00

2

1.11E+00

1.10E+00

1.10E+00

1.09E+00

1.11E+00

1.16E+00

1.10E+00

3

1.10E+00

1.11E+00

1.11E+00

1.10E+00

1.12E+00

1.12E+00

1.08E+00

5

1.12E+00

1.08E+00

1.07E+00

1.09E+00

1.10E+00

1.06E+00

1.09E+00

7

1.08E+00

1.06E+00

1.07E+00

1.08E+00

1.07E+00

1.06E+00

1.07E+00

10

1.06E+00

1.06E+00

1.07E+00

1.06E+00

1.04E+00

1.04E+00

1.05E+00

15

1.08E+00

1.03E+00

1.03E+00

1.06E+00

1.05E+00

1.06E+00

1.05E+00

20

1.07E+00

9.99E-01

1.03E+00

1.04E+00

1.02E+00

1.04E+00

1.04E+00

30

1.04E+00

1.01E+00

1.01E+00

1.03E+00

1.02E+00

1.01E+00

1.01E+00

50

1.01E+00

1.00E+00

9.98E-01

1.03E+00

1.00E+00

9.95E-01

1.01E+00

FINAL DRAFT JULY 2017

1688
1689

NOT TO BE REFERENCED

Table A.5.4.2b Conversion coefficient from photon air kerma to personal absorbed dose in local skin on
the pillar phantom calculated using the kerma-approximation method (2/2) (Otto, 2017).
dp local skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

1690
1691
1692
1693
1694
1695
1696
1697
1698
1699
1700

0.002

105
0.00E+00120
0.00E+00135
0.00E+00

150
0.00E+00

165
0.00E+00

180
0.00E+00

ROT
3.32E-03

0.003

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

7.28E-02

0.004

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

1.80E-01

0.005

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.75E-01

0.007

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.88E-01

0.01

6.21E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

4.60E-01

0.015

6.21E-02

3.75E-03

2.60E-04

4.45E-05

8.99E-06

1.05E-05

5.25E-01

0.02

2.61E-01

6.97E-02

2.25E-02

1.02E-02

6.08E-03

4.66E-03

5.97E-01

0.03

6.39E-01

3.71E-01

2.32E-01

1.73E-01

1.41E-01

1.28E-01

7.89E-01

0.05

1.00E+00

7.27E-01

5.73E-01

4.60E-01

4.19E-01

4.37E-01

1.05E+00

0.07

1.08E+00

8.31E-01

6.82E-01

5.92E-01

5.28E-01

5.28E-01

1.11E+00

0.1

1.08E+00

8.63E-01

7.07E-01

6.32E-01

5.73E-01

5.71E-01

1.09E+00

0.15

1.08E+00

8.80E-01

7.53E-01

6.57E-01

6.12E-01

5.89E-01

1.07E+00

0.2

1.07E+00

8.73E-01

7.58E-01

6.81E-01

6.32E-01

6.27E-01

1.05E+00

0.3

1.05E+00

9.11E-01

8.11E-01

7.19E-01

6.86E-01

6.83E-01

1.04E+00

0.5

1.07E+00

9.38E-01

8.42E-01

7.89E-01

7.63E-01

7.33E-01

1.04E+00

0.662

1.07E+00

9.41E-01

8.62E-01

8.09E-01

7.89E-01

7.55E-01

1.03E+00

0.7

1.07E+00

9.49E-01

8.68E-01

8.16E-01

7.83E-01

7.67E-01

1.03E+00

1

1.05E+00

9.78E-01

8.78E-01

8.45E-01

8.35E-01

8.18E-01

1.03E+00

1.25

1.06E+00

9.92E-01

9.25E-01

8.83E-01

8.44E-01

8.35E-01

1.04E+00

1.5

1.06E+00

9.87E-01

9.29E-01

9.08E-01

8.72E-01

8.80E-01

1.04E+00

2

1.07E+00

9.83E-01

9.45E-01

9.03E-01

8.99E-01

8.81E-01

1.04E+00

3

1.07E+00

1.02E+00

9.53E-01

9.53E-01

9.07E-01

9.25E-01

1.05E+00

5

1.07E+00

1.03E+00

9.76E-01

9.48E-01

9.46E-01

9.46E-01

1.04E+00

7

1.03E+00

9.96E-01

9.57E-01

9.81E-01

9.33E-01

9.42E-01

1.03E+00

10

1.02E+00

1.01E+00

9.85E-01

9.46E-01

9.47E-01

9.41E-01

1.02E+00

15

1.01E+00

9.94E-01

9.65E-01

9.13E-01

9.50E-01

9.24E-01

1.01E+00

20

1.00E+00

9.85E-01

9.44E-01

9.40E-01

9.15E-01

9.23E-01

9.95E-0130

9.68E-01

9.46E-01

9.48E-01

9.33E-01

9.34E-01

8.95E-01

9.82E-0150

9.58E-01

9.43E-01

9.19E-01

8.86E-01

8.65E-01

8.65E-01

9.62E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1701
1702
1703
1704
1705
1706
1707
1708
1709
1710
1711
1712
1713
1714
1715
1716
1717
1718
1719
1720
1721
1722
1723
1724
1725
1726
1727
1728
1729
1730
1731
1732
1733
1734
1735
1736
1737
1738
1739
1740
1741
1742
1743
1744
1745
1746

Figure A.5.4.2b Conversion coefficient from photon air kerma to personal absorbed dose in local
skin on the pillar phantom calculated using the kerma-approximation method (Otto, 2017).

FINAL DRAFT JULY 2017

1747
1748

NOT TO BE REFERENCED

Table A.5.4.3a Conversion coefficient from photon fluence to personal absorbed dose in local skin on
the rod phantom calculated using the kerma-approximation method (1/2) (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1749
1750
1751
1752

0.002

0
2.54E+00

15
2.28E+0030
1.63E+00

45
9.08E-0160
3.63E-0175
8.56E-0290
0.00E+00

0.003

1.97E+01

1.87E+01

1.58E+01

1.14E+01

6.66E+00

2.91E+00

7.39E-01

0.004

2.56E+01

2.49E+01

2.29E+01

1.90E+01

1.32E+01

7.35E+00

2.84E+00

0.005

2.24E+01

2.21E+01

2.10E+01

1.88E+01

1.45E+01

9.19E+00

4.36E+00

0.007

1.39E+01

1.39E+01

1.36E+01

1.30E+01

1.14E+01

8.19E+00

4.71E+00

0.01

7.21E+00

7.20E+00

7.15E+00

7.04E+00

6.64E+00

5.39E+00

3.62E+00

0.015

3.21E+00

3.21E+00

3.20E+00

3.18E+00

3.12E+00

2.84E+00

2.30E+00

0.02

1.81E+00

1.81E+00

1.80E+00

1.79E+00

1.77E+00

1.69E+00

1.50E+00

0.03

8.16E-01

8.15E-01

8.13E-01

8.10E-01

8.04E-01

7.84E-01

7.42E-01

0.05

3.79E-01

3.80E-01

3.80E-01

3.81E-01

3.80E-01

3.74E-01

3.59E-01

0.06

3.42E-01

3.42E-01

3.42E-01

3.41E-01

3.40E-01

3.36E-01

3.25E-01

0.07

3.46E-01

3.44E-01

3.43E-01

3.42E-01

3.40E-01

3.37E-01

3.28E-01

0.1

4.43E-01

4.43E-01

4.43E-01

4.43E-01

4.42E-01

4.38E-01

4.26E-01

0.15

6.98E-01

6.98E-01

6.98E-01

6.99E-01

7.00E-01

6.98E-01

6.86E-01

0.2

9.90E-01

9.87E-01

9.87E-01

9.87E-01

9.88E-01

9.87E-01

9.71E-01

0.5

2.67E+00

2.67E+00

2.67E+00

2.67E+00

2.68E+00

2.68E+00

2.65E+00

0.662

3.49E+00

3.49E+00

3.49E+00

3.49E+00

3.49E+00

3.49E+00

3.46E+00

1

4.98E+00

4.97E+00

4.97E+00

4.98E+00

4.98E+00

4.98E+00

4.95E+00

1.25

5.93E+00

5.93E+00

5.94E+00

5.95E+00

5.96E+00

5.95E+00

5.92E+00

1.5

6.78E+00

6.79E+00

6.79E+00

6.80E+00

6.81E+00

6.80E+00

6.77E+00

2

8.31E+00

8.32E+00

8.32E+00

8.32E+00

8.34E+00

8.33E+00

8.30E+00

3

1.09E+01

1.09E+01

1.09E+01

1.09E+01

1.10E+01

1.09E+01

1.09E+01

5

1.53E+01

1.54E+01

1.54E+01

1.54E+01

1.54E+01

1.53E+01

1.53E+01

10

2.56E+01

2.56E+01

2.55E+01

2.55E+01

2.55E+01

2.55E+01

2.54E+01

20

4.68E+01

4.68E+01

4.68E+01

4.66E+01

4.65E+01

4.65E+01

4.65E+0130

6.91E+01

6.92E+01

6.91E+01

6.91E+01

6.91E+01

6.90E+01

6.87E+0150

1.19E+02

1.19E+02

1.19E+02

1.19E+02

1.19E+02

1.19E+02

1.18E+02

FINAL DRAFT JULY 2017

1753
1754

NOT TO BE REFERENCED

Table A.5.4.3a Conversion coefficient from photon fluence to personal absorbed dose in local skin on
the rod phantom calculated using the kerma-approximation method (2/2) (Otto, 2017).
dp local skin / (pGy cm2) for a radiation incidence at 
Ep / MeV

1755
1756

0.002

105
0.00E+00120
0.00E+00135
0.00E+00

150
0.00E+00

165
0.00E+00

180
0.00E+00

ROT
5.45E-01

0.003

4.70E-02

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

5.51E+00

0.004

4.54E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

8.62E+00

0.005

1.09E+00

1.93E-02

0.00E+00

0.00E+00

0.00E+00

0.00E+00

8.52E+00

0.007

1.77E+00

1.72E-01

0.00E+00

0.00E+00

0.00E+00

0.00E+00

6.14E+00

0.01

1.83E+00

4.98E-01

5.45E-02

0.00E+00

0.00E+00

0.00E+00

3.59E+00

0.015

1.61E+00

9.40E-01

5.00E-01

2.93E-01

2.05E-01

1.80E-01

1.92E+00

0.02

1.24E+00

9.51E-01

7.19E-01

5.79E-01

5.05E-01

4.81E-01

1.29E+00

0.03

6.77E-01

6.02E-01

5.35E-01

4.87E-01

4.59E-01

4.50E-01

6.80E-01

0.05

3.38E-01

3.14E-01

2.93E-01

2.78E-01

2.70E-01

2.67E-01

3.39E-01

0.06

3.09E-01

2.90E-01

2.72E-01

2.60E-01

2.52E-01

2.50E-01

3.09E-01

0.07

3.14E-01

2.95E-01

2.78E-01

2.65E-01

2.57E-01

2.55E-01

3.12E-01

0.1

4.09E-01

3.88E-01

3.69E-01

3.54E-01

3.46E-01

3.43E-01

4.08E-01

0.15

6.66E-01

6.37E-01

6.08E-01

5.86E-01

5.73E-01

5.69E-01

6.57E-01

0.2

9.43E-01

9.06E-01

8.70E-01

8.45E-01

8.28E-01

8.23E-01

9.34E-01

0.5

2.60E+00

2.53E+00

2.47E+00

2.42E+00

2.39E+00

2.38E+00

2.58E+00

0.662

3.41E+00

3.33E+00

3.26E+00

3.20E+00

3.17E+00

3.16E+00

3.38E+00

1

4.88E+00

4.80E+00

4.72E+00

4.65E+00

4.59E+00

4.58E+00

4.85E+00

1.25

5.84E+00

5.75E+00

5.66E+00

5.59E+00

5.55E+00

5.54E+00

5.82E+00

1.5

6.70E+00

6.61E+00

6.52E+00

6.44E+00

6.39E+00

6.37E+00

6.67E+00

2

8.23E+00

8.12E+00

8.02E+00

7.95E+00

7.92E+00

7.92E+00

8.19E+00

3

1.08E+01

1.07E+01

1.06E+01

1.05E+01

1.05E+01

1.05E+01

1.08E+01

5

1.52E+01

1.51E+01

1.50E+01

1.49E+01

1.48E+01

1.48E+01

1.52E+01

10

2.53E+01

2.52E+01

2.50E+01

2.49E+01

2.48E+01

2.47E+01

2.53E+01

20

4.64E+01

4.61E+01

4.58E+01

4.56E+01

4.55E+01

4.54E+01

4.63E+0130

6.85E+01

6.80E+01

6.76E+01

6.75E+01

6.74E+01

6.75E+01

6.85E+0150

1.17E+02

1.16E+02

1.16E+02

1.15E+02

1.14E+02

1.15E+02

1.17E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1757
1758
1759
1760
1761
1762
1763
1764
1765
1766
1767
1768
1769
1770
1771
1772
1773
1774
1775
1776
1777
1778
1779
1780
1781
1782
1783
1784
1785
1786
1787
1788
1789
1790
1791
1792
1793
1794
1795
1796
1797
1798
1799
1800

Figure A.5.4.3a Conversion coefficient from photon fluence to personal absorbed dose in local
skin on the rod phantom calculated using the kerma-approximation method (Otto, 2017).

FINAL DRAFT JULY 2017

1801
1802

NOT TO BE REFERENCED

Table A.5.4.3b Conversion coefficients from photon air kerma to personal absorbed dose in local skin on
the rod phantom calculated using the kerma-approximation method (1/2) (Otto, 2017).
dp local skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

1803
1804

0.002

0
1.55E-0215
1.39E-0230
9.96E-0345
5.55E-0360
2.22E-0375
5.23E-0490
0.00E+00

0.003

2.62E-01

2.48E-01

2.10E-01

1.51E-01

8.84E-02

3.86E-02

9.81E-03

0.004

5.38E-01

5.23E-01

4.81E-01

3.99E-01

2.77E-01

1.54E-01

5.96E-02

0.005

7.31E-01

7.21E-01

6.85E-01

6.13E-01

4.73E-01

3.00E-01

1.42E-01

0.007

8.97E-01

8.97E-01

8.77E-01

8.39E-01

7.35E-01

5.28E-01

3.04E-01

0.01

9.74E-01

9.73E-01

9.66E-01

9.51E-01

8.97E-01

7.28E-01

4.89E-01

0.015

1.03E+00

1.03E+00

1.02E+00

1.02E+00

9.98E-01

9.09E-01

7.36E-01

0.02

1.07E+00

1.07E+00

1.07E+00

1.06E+00

1.05E+00

1.00E+00

8.91E-01

0.03

1.13E+00

1.13E+00

1.13E+00

1.12E+00

1.11E+00

1.09E+00

1.03E+00

0.05

1.17E+00

1.18E+00

1.18E+00

1.18E+00

1.18E+00

1.16E+00

1.11E+00

0.06

1.18E+00

1.18E+00

1.18E+00

1.18E+00

1.18E+00

1.16E+00

1.12E+00

0.07

1.20E+00

1.20E+00

1.19E+00

1.19E+00

1.18E+00

1.17E+00

1.14E+00

0.1

1.19E+00

1.19E+00

1.19E+00

1.19E+00

1.19E+00

1.18E+00

1.15E+00

0.15

1.16E+00

1.16E+00

1.16E+00

1.17E+00

1.17E+00

1.16E+00

1.14E+00

0.2

1.16E+00

1.15E+00

1.15E+00

1.15E+00

1.15E+00

1.15E+00

1.13E+00

0.5

1.12E+00

1.12E+00

1.12E+00

1.12E+00

1.13E+00

1.13E+00

1.11E+00

0.662

1.12E+00

1.12E+00

1.12E+00

1.12E+00

1.12E+00

1.12E+00

1.11E+00

1

1.11E+00

1.11E+00

1.11E+00

1.11E+00

1.11E+00

1.11E+00

1.10E+00

1.25

1.11E+00

1.11E+00

1.11E+00

1.12E+00

1.12E+00

1.12E+00

1.11E+00

1.5

1.10E+00

1.10E+00

1.10E+00

1.11E+00

1.11E+00

1.11E+00

1.10E+00

2

1.10E+00

1.10E+00

1.10E+00

1.10E+00

1.10E+00

1.10E+00

1.10E+00

3

1.09E+00

1.09E+00

1.09E+00

1.09E+00

1.10E+00

1.09E+00

1.09E+00

5

1.08E+00

1.09E+00

1.09E+00

1.09E+00

1.09E+00

1.08E+00

1.08E+00

10

1.06E+00

1.06E+00

1.06E+00

1.06E+00

1.06E+00

1.06E+00

1.05E+00

20

1.03E+00

1.03E+00

1.03E+00

1.03E+00

1.03E+00

1.03E+00

1.03E+00

30

1.01E+00

1.01E+00

1.01E+00

1.01E+00

1.01E+00

1.01E+00

1.00E+00

50

9.98E-01

9.98E-01

9.98E-01

9.98E-01

9.98E-01

9.98E-01

9.90E-01

FINAL DRAFT JULY 2017

1805
1806

NOT TO BE REFERENCED

Table A.5.4.3b Conversion coefficient from photon air kerma to personal absorbed dose in local skin on
the rod phantom calculated using the kerma-approximation method (2/2) (Otto, 2017).
dp local skin / (GyGy-1) for a radiation incidence at 
Ep / MeV

1807
1808

0.002

105
0.00E+00120
0.00E+00135
0.00E+00

150
0.00E+00

165
0.00E+00

180
0.00E+00

ROT
3.33E-03

0.003

6.24E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

7.32E-02

0.004

9.53E-03

0.00E+00

0.00E+00

0.00E+00

0.00E+00

0.00E+00

1.81E-01

0.005

3.56E-02

6.30E-04

0.00E+00

0.00E+00

0.00E+00

0.00E+00

2.78E-01

0.007

1.14E-01

1.11E-02

0.00E+00

0.00E+00

0.00E+00

0.00E+00

3.96E-01

0.01

2.47E-01

6.73E-02

7.36E-03

0.00E+00

0.00E+00

0.00E+00

4.85E-01

0.015

5.15E-01

3.01E-01

1.60E-01

9.38E-02

6.56E-02

5.76E-02

6.14E-01

0.02

7.36E-01

5.65E-01

4.27E-01

3.44E-01

3.00E-01

2.86E-01

7.66E-01

0.03

9.38E-01

8.34E-01

7.41E-01

6.75E-01

6.36E-01

6.24E-01

9.42E-01

0.05

1.05E+00

9.72E-01

9.07E-01

8.61E-01

8.36E-01

8.27E-01

1.05E+00

0.06

1.07E+00

1.00E+00

9.42E-01

9.00E-01

8.72E-01

8.65E-01

1.07E+00

0.07

1.09E+00

1.03E+00

9.66E-01

9.21E-01

8.93E-01

8.86E-01

1.08E+00

0.1

1.10E+00

1.04E+00

9.94E-01

9.53E-01

9.32E-01

9.24E-01

1.10E+00

0.15

1.11E+00

1.06E+00

1.01E+00

9.78E-01

9.56E-01

9.49E-01

1.10E+00

0.2

1.10E+00

1.06E+00

1.02E+00

9.86E-01

9.66E-01

9.61E-01

1.09E+00

0.5

1.09E+00

1.06E+00

1.04E+00

1.02E+00

1.00E+00

1.00E+00

1.08E+00

0.662

1.10E+00

1.07E+00

1.05E+00

1.03E+00

1.02E+00

1.02E+00

1.09E+00

1

1.09E+00

1.07E+00

1.05E+00

1.04E+00

1.02E+00

1.02E+00

1.08E+00

1.25

1.10E+00

1.08E+00

1.06E+00

1.05E+00

1.04E+00

1.04E+00

1.09E+00

1.5

1.09E+00

1.08E+00

1.06E+00

1.05E+00

1.04E+00

1.04E+00

1.09E+00

2

1.09E+00

1.07E+00

1.06E+00

1.05E+00

1.05E+00

1.05E+00

1.08E+00

3

1.08E+00

1.07E+00

1.06E+00

1.05E+00

1.05E+00

1.05E+00

1.08E+00

5

1.07E+00

1.06E+00

1.06E+00

1.05E+00

1.04E+00

1.04E+00

1.07E+00

10

1.05E+00

1.04E+00

1.04E+00

1.03E+00

1.03E+00

1.02E+00

1.05E+00

20

1.02E+00

1.02E+00

1.01E+00

1.01E+00

1.00E+00

1.00E+00

1.02E+00

30

9.99E-01

9.91E-01

9.86E-01

9.84E-01

9.83E-01

9.84E-01

9.99E-0150

9.82E-01

9.73E-01

9.73E-01

9.65E-01

9.56E-01

9.65E-01

9.82E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1809
1810
1811
1812
1813
1814
1815
1816
1817
1818
1819
1820
1821
1822
1823
1824
1825
1826
1827
1828
1829
1830
1831
1832
1833
1834
1835
1836
1837
1838
1839
1840
1841
1842
1843
1844
1845
1846
1847
1848
1849
1850
1851
1852

Figure A.5.4.3b Conversion coefficient from photon air kerma to personal absorbed dose in local
skin on the rod phantom calculated using the kerma-approximation method (Otto, 2017).

FINAL DRAFT JULY 2017

1853

NOT TO BE REFERENCED

A.6 Air Kerma

1854

The Table gives values of conversion coefficients from photon fluence to air kerma for energies from

1855

2keV to 50 MeV. Air kerma coefficients, Kair/Φ = (µen/ρ) E (1-g)-1are used for the conversion from dose1856

per fluence to dose per air kerma. The values for (µen/ ρ) are from the calculations of Seltzer (1993) and1857

Hubbell and Seltzer (1995) with renormalized Scoﬁeld photoeffect cross sections (ICRU, 2014). The

1858

values for g are from Seltzer (2017). The values written in bold italics are obtained by interpolation as

1859

no values for (µen/ ρ) are availablea).

1860
1861
1862

FINAL DRAFT JULY 2017

1863

Table A.6 Conversion coefficients from photon fluence to air kerma.
Photon energy E
(MeV)
0.002
0.003
0.004
0.005
0.006
0.007
0.008
0.009
0.010
0.011
0.012
0.013
0.015
0.017
0.020
0.024
0.025
0.030
0.040
0.050
0.060
0.070
0.080
0.100
0.120
0.150
0.200
0.240
0.300
0.400

1864
1865
1866

NOT TO BE REFERENCEDa)

Air kermacoefficient(pGy cm²)

Photon energy E
(MeV)

163.7
75.32
47.62
30.65
21.25
15.50
11.79
9.221
7.400
6.043
5.022
4.236
3.125
2.388
1.684
1.150
1.056
0.72170.42890.32290.28890.28780.30670.37140.4606
0.59940.8567
1.062
1.383
1.892

0.500
0.511
0.600
0.662
0.700
0.800
1.000
1.117
1.200
1.250
1.300
1.330
1.500
1.700
2.000
2.400
3.000
4.000
5.000
6.000
6.129
7.000
8.000
10.00015.00020.00030.00040.00050.000Air kermacoefficient(pGy cm²)

2.379
2.431
2.844
3.112
3.275
3.702
4.481
4.884
5.165
5.332
5.498
5.596
6.147
6.725
7.557
8.563
9.977
12.14
14.18
16.17
16.44
18.19
20.13
24.13
34.46
45.36
68.59
93.29
119.2

A log-log-interpolation was used except for 70 keV: At this energy, the values take a minimum resulting in a
curved energy dependence. Therefore, a natural cubic spline was used for this energy.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1867
1868

Appendix B

1869

Descriptions of codes

1870

B.1 PHITS

1871

The PHITS (Particle and Heavy Ion Transport Code System) code is a multipurpose Monte

1872

Carlo code that simulates the transport and interaction of hadrons, leptons, and heavy ions in arbitrary

1873

three-dimensional geometries (Sato et al., 2013). PHITS 2.82 was used in this report.

1874

In the PHITS code, neutron transport below 20 MeV down to 10 -5 eV is simulated in a manner

1875

similar to that employed in the MCNP4C code (Briesmeister, 2000), and is based on evaluated1876

nuclear data libraries. For neutrons above 20 MeV and for protons, mesons, and other hadrons up to1877

200 GeV, the intra-nuclear cascade models INCL4.6 (Boudard et al., 2013) and JAM (Nara et al.,1878

1999) are employed for simulating the dynamic stage of hadron-induced nuclear reactions in the1879

intermediate and high energy regions, respectively. Nucleus-induced reactions are simulated by the

1880

JQMD model (Niita et al, 1995) for energies from 10 MeV/u up to 100 GeV/u. The evaporation and1881

fission model GEM (Furihata, 2000) is adopted for simulating the static stage for both hadron- and1882

nucleus-induced reactions. The energy losses of charged particles, except for electrons, are calculated

1883

using the SPAR (Armstrong and Chandler, 1973) or ATIMA (Geissel et al., 2013) codes with the1884continuous slowing down approximation.

1885
1886

Transport of photons and electrons are simulated in a similar way as in the EGS5 (Hirayama
et al., 2005) code. Photo-nuclear reactions can be treated up to 1 GeV using JQMD and GEM.

1887

The PHITS code is capable of: (1) providing good estimations of generated particle spectra

1888

produced from nucleon–nucleus and nucleus–nucleus collisions using the INCL4.6, JAM and JQMD

1889

models; (2) determining the energy of charged particles emitted from low-energy neutron-induced

1890

nuclear reactions using the event generator mode, instead of the kerma approximation; and (3)1891estimating the probability density of absorbed dose in terms of LET and lineal energy.

FINAL DRAFT JULY 2017

1892
1893

NOT TO BE REFERENCED

B.2 FLUKA
FLUKA is a general-purpose Monte Carlo program for calculations of particle and photon

1894

transport (Böhlen et al., 2014; Ferrari et al., 2005) that can simulate the interactions and propagation

1895

of approximately 60 different particles in matter, including heavy ions. Photonuclear interactions can

1896

be simulated. FLUKA 2011 was used in this report.

1897

Depending on the energies of the primary particles, hadronic interactions are simulated by1898

different physical models (Ballarini et al., 2004). For higher energies, the Dual Parton model is used.

1899

Below 3–5 GeV c-1, the PEANUT (Cascade–Pre-equilibrium model) package includes a very

1900

detailed generalized intra-nuclear cascade (GINC) and a pre-equilibrium stage, while at high1901

energies, the Gribov-Glauber multiple collision mechanism is included in a less-refined GINC.

1902

Nuclear interactions generated by ions are treated through interfaces to external event generators,

1903

except for the low-energy (<150 MeV/u) range for which a model based on the Boltzmann master

1904

equation has been implemented. The relativistic quantum molecular dynamics generator is invoked

1905

from 100 MeV/u to 5 GeV/u, and the DPMJET code is used for energies over 5 GeV/u.

1906

The transport of charged particles is described by applying a multiple scattering algorithm

1907

based on Moliere’s theory of Coulomb scattering. The algorithm includes an accurate treatment of1908

curved trajectories in magnetic fields. The energy loss is determined according to the Bethe–Bloch1909

theory and from bremsstrahlung and pair production. Ionization fluctuations are accounted for.

1910

For neutrons with energies lower than 20 MeV, FLUKA employs a multigroup transport

1911

algorithm that uses a subdivision of the neutron energy range in 260 groups and is based on neutron

1912

cross section libraries containing more than 200 different materials, selected for their use in physics,

1913

dosimetry, and accelerator engineering. Energy depositions for nuclei other than hydrogen are

1914

calculated by kerma coefficients.

1915

B.3 MCNP6

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1916

The particle radiation transport code Monte Carlo N-Particle (MCNP)is a general purpose

1917

three-dimensional simulation tool that transports 37 different particle types. It can be applied in1918

many applications including radiation protection and dosimetry, radiation shielding, radiography,

1919

medical physics, nuclear criticality safety, detector design and analysis, accelerator target design,

1920

fission and fusion reactor design, decontamination and decommissioning. The specific release of the1921

code used in this report was version 6.1. (Pelowitz et al. 2013)The code covers the following

1922

ranges:10-11 MeV to 20 MeV for neutrons with data up to 150 MeV for some nuclides, 1 keV to 1

1923

GeV for electrons (and positrons), and 1 keV to 100 GeV for photons.

1924

Neutron, proton, electron and photon are transported using tabulated data below an upper

1925

energy table limit. That upper energy limit varies with nuclide and cross section data requested.

1926

Above that upper energy limit, a combination of models can be used to describe the transport and1927

reactions. The reader is referred to (Goorley et al. 2013) for more details on the models available for1928

use it.

1929

The neutron calculations in the report performed with MCNP6, version 1.0, used pointwise

1930

cross-section. In the present calculations, the S(α,β) thermal neutron scattering model for water was1931

used in the computations of neutron skin doses and lens of the eye doses. If available, nuclide cross1932

section tables extending to 150 MeV were used for the computations at 30 MeV and 50 MeV. The

1933

code mix and matches tabulated cross section library data and physics models as needed to cover the1934

energy ranges of the computation. The neutron library data used in the present computations is1935

shown in Table B.1; the tabulated cross section with the latest evaluation was selected for this work.

1936

For photons, the code accounts for incoherent and coherent scattering, the possibility of1937

fluorescent emission after photoelectric absorption, absorption in pair production with local emission

1938

of annihilation radiation, and bremsstrahlung. A continuous-slowing-down model is used for electron

1939

transport that includes positrons, k x-rays, and bremsstrahlung. Photonuclear physics is available for1940

a subset of umber of nuclides

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1941

MCNP contains numerous flexible tallies: surface current & flux (surface crossing), volume flux

1942

(track length), point or ring detectors, particle heating, fission heating, pulse height tally for energy or1943

charge deposition, mesh tallies, and radiography tallies.

1944

Neutron Cross Sections Used in MCNP6 Computations. (J. L. Conlin et al. 2005)
NuclideMCNP
Identifier

Source (Upper Energy Limit ofData Tables)

H-1

1001.62c

ENDF/B-VI.8 (150 MeV)

H-2

1002.80c

ENDF/B-VII.1 (150 MeV)

Natural Carbon

6000.80c

ENDF/B-VII.1 (150 MeV)

N-14

7014.80c

ENDF/B-VII.1 (150 MeV)

N-15

7015.80c

ENDF/B-VII.1 (20 MeV)

O-16

8016.80c

ENDF/B-VII.1 (150 MeV)

O-17

8017.80c

ENDF/B-VII.1 (150 MeV)

Na-23

11023.80c

ENDF/B-VII.1 (20 MeV)

P-31

15031.80c

ENDF/B-VII.1 (150 MeV)

S-32

16032.80c

ENDF/B-VII.1 (20 MeV)

S-33

16033.80c

ENDF/B-VII.1 (20 MeV)

S-35

16035.80c

ENDF/B-VII.1 (20 MeV)

S-36

16036.80c

ENDF/B-VII.1 (20 MeV)

Cl-35

17035.80c

ENDF/B-VII.1 (20 MeV)

Cl-37

17037.80c

ENDF/B-VII.1 (20 MeV)

K-39

19039.80c

ENDF/B-VII.1 (20 MeV)

K-40

19040.80c

ENDF/B-VII.1 (20 MeV)

K-41

19041.80c

ENDF/B-VII.1 (20 MeV)

1945
1946

B.4 EGSnrc

1947

For the calculations presented in this report, the electron-gamma-shower code system EGSnrc

1948

Version v4-r2-4-0 (Kawrakow et al., 2013) has been used. This code is an extended and improved

1949

version of EGS4 (Nelson et al., 1985), maintained by the National Research Council of Canada

1950(NRC). The transport of photons, electrons, and positrons can be simulated for particle kinetic

1951

energies from a few keV up to several hundred GeV. Some enhancements to the physics, however,1952

can only be enabled below 1 GeV.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1953

For photon transport, bound Compton scattering and photo-electrons fromK, L, and M shells

1954

are considered for all energies. In both cases, resulting fluorescence or Auger and Coster-Kronig

1955

electrons are followed. Photon–nuclear reactions are not taken into consideration as their contribution

1956

to organ dose was shown to be much less than 1%. In this report, photon transport is terminated when1957

the photon energy falls below 10keV.Exceptions are used for primary particles with an initial kinetic

1958

energy below 510 keV, whose histories are followed down to 1keV.

1959

Electron and positron transport calculations are performed by a Class II condensed history

1960

technique (Berger, 1963), which transports generated particles produced above a certain chosen

1961energy. Bremsstrahlung cross sections are those from Bethe-Heitler, i.e. as in EGS4 (Nelson et al.,

19621985). Bremsstrahlung angular sampling following Koch and Motz (1959) is used. Electron impact

1963

ionization is modeled using default cross sections (Kawrakow, 2002). When the sampling does not

1964lead to ionization, the classical Møller or Bhabha cross sections are applied. For elastic scattering,1965

spin effects are taken into account. Pair production is simulated as in EGS4 (Nelson et al., 1985).

1966

Triplet-production processes are neglected for all particles. In this report, the transport history of1967electrons is generally terminated when their kinetic energy falls below 10keV. Exceptions are used1968

for primary particles with an initial kinetic energy below 110keV, whose histories are followed down

1969

to 1keV. For external irradiation, electrons with kinetic energies below 500 keV rarely reach internal

1970

organs. The dose to those organs is low and mainly caused by bremsstrahlung production within the1971

first few millimetres of the phantoms.

1972

B.5 Revised Stopping Powers

1973

The ICRU Report 90 Key Data for Ionizing-Radiation Dosimetry: Measurement Standards and1974

Applications, (ICRU, 2017) has changed slightly the charged-particle stopping powers in water. This1975

is not expected to make a noticeable difference to the Monte Carlo calculations used in this Report.

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1976

Appendix C

1977

Informative: Alternative Conversion Coefficients to Absorbed Dose to the Lens of the Eye

1978

C.1 Directional and Personal Absorbed Dose to the Lens of the Eye, Maximum Absorbed Dose to

1979

the Sensitive cells or the Complete Lens

1980

The numerical values of conversion coefficients from particle fluence to directional absorbed dose in1981

the lens of the eye d'lens max and from fluence to personal absorbed dose in the lens of the eye dplens max are

1982

the same and the symbol dlens max, is used in the following Tables. The conversion coefficients given here1983

are to the maximum value of the absorbed dose in the radiation sensitive cells or the complete lens of

1984

the eye, calculated for whole-body exposure of the stylized eye model (Behrens and Dietze, 2011) for

1985

broad parallel beams incident for angles from 0° (A-P) to 90° in 15° steps, the maximum value of right1986

or left irradiations is taken; and for a rotational field (ROT).

1987

Tables C.1.1a to C.1.4, and Figures C.1.1a to C.1.4 give the numerical values of the conversion

1988

coefficients from particle fluence for photons, neutrons, electrons, and positrons for energies up to 50

1989

MeV; Table C.1.1b and Figure C.1.1b from air kerma.

1990

FINAL DRAFT JULY 2017

1991
1992

NOT TO BE REFERENCED

Table C.1.1a Conversion coefficients from photon fluence to the maximum absorbed dose in thesensitive cells or the complete lens for left or right irradiations (Behrens, 2017a).
dlens, max (α )/ (pGy cm2) for a radiation incidence at 

Ep / MeV
0.005
0.006
0.007
0.008
0.009
0.01
0.011
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.12
0.15
0.2
0.24
0.3
0.4
0.5
0.511
0.6
0.662
0.8
1
1.117
1.2
1.3
1.33
1.5
1.7
2
2.4
3
4
5
6
6.129
8
10
15
20
30
40
50

0

15

30

45

60

75

90

ROT

4.17E-05
7.75E-03
1.13E-01
4.46E-01
9.37E-01
1.42E+00
1.75E+00
2.01E+00
1.94E+00
1.76E+00
1.45E+00
1.14E+00
8.26E-01
5.80E-01
4.83E-01
4.50E-01
4.55E-01
4.82E-01
5.59E-01
6.66E-01
8.38E-01
1.13E+00
1.39E+00
1.74E+00
2.29E+00
2.83E+00
2.88E+00
3.34E+00
3.63E+00
4.26E+00
5.06E+00
5.50E+00
5.83E+00
6.07E+00
6.16E+00
6.59E+00
6.92E+00
7.04E+00
6.84E+00
6.35E+00
5.62E+00
5.13E+00
4.82E+00
4.79E+00
4.42E+00
4.17E+00
3.97E+00
3.94E+00
4.01E+00
4.09E+00
4.16E+00

7.65E-05
9.30E-03
1.07E-01
4.12E-01
8.79E-01
1.34E+00
1.68E+00
1.99E+00
1.96E+00
1.79E+00
1.49E+00
1.16E+00
8.54E-01
5.96E-01
4.94E-01
4.63E-01
4.63E-01
4.83E-01
5.62E-01
6.70E-01
8.42E-01
1.15E+00
1.40E+00
1.75E+00
2.32E+00
2.84E+00
2.90E+00
3.36E+00
3.65E+00
4.28E+00
5.09E+00
5.55E+00
5.84E+00
6.14E+00
6.26E+00
6.63E+00
6.93E+00
7.16E+00
6.93E+00
6.49E+00
5.85E+00
5.35E+00
5.05E+00
5.06E+00
4.67E+00
4.38E+00
4.16E+00
4.08E+00
4.12E+00
4.18E+00
4.32E+00

1.54E-04
1.06E-02
1.05E-01
3.77E-01
8.00E-01
1.23E+00
1.57E+00
1.89E+00
1.89E+00
1.74E+00
1.48E+00
1.16E+00
8.45E-01
6.03E-01
5.04E-01
4.69E-01
4.67E-01
4.89E-01
5.69E-01
6.72E-01
8.46E-01
1.17E+00
1.41E+00
1.77E+00
2.34E+00
2.89E+00
2.97E+00
3.40E+00
3.66E+00
4.33E+00
5.14E+00
5.56E+00
5.86E+00
6.16E+00
6.26E+00
6.71E+00
7.08E+00
7.29E+00
7.24E+00
6.92E+00
6.43E+00
6.08E+00
5.87E+00
5.76E+00
5.52E+00
5.19E+00
4.78E+00
4.60E+00
4.58E+00
4.68E+00
4.71E+00

1.52E-04
1.05E-02
9.55E-02
3.37E-01
7.04E-01
1.09E+00
1.41E+00
1.73E+00
1.75E+00
1.64E+00
1.39E+00
1.12E+00
8.17E-01
5.89E-01
4.96E-01
4.64E-01
4.63E-01
4.85E-01
5.72E-01
6.79E-01
8.45E-01
1.17E+00
1.42E+00
1.83E+00
2.38E+00
2.93E+00
3.02E+00
3.46E+00
3.77E+00
4.39E+00
5.27E+00
5.65E+00
5.98E+00
6.35E+00
6.40E+00
6.88E+00
7.25E+00
7.66E+00
7.84E+00
7.87E+00
7.67E+00
7.68E+00
7.60E+00
7.62E+00
7.47E+00
7.16E+00
6.58E+00
6.15E+00
5.84E+00
5.69E+00
5.70E+00

6.90E-05
5.87E-03
6.16E-02
2.37E-01
5.20E-01
8.49E-01
1.15E+00
1.54E+00
1.62E+00
1.55E+00
1.36E+00
1.10E+00
8.27E-01
5.92E-01
4.95E-01
4.61E-01
4.61E-01
4.90E-01
5.70E-01
6.71E-01
8.48E-01
1.15E+00
1.40E+00
1.79E+00
2.36E+00
2.96E+00
3.02E+00
3.47E+00
3.73E+00
4.44E+00
5.24E+00
5.64E+00
5.95E+00
6.31E+00
6.45E+00
6.91E+00
7.40E+00
7.92E+00
8.47E+00
8.99E+00
9.64E+00
1.01E+01
1.07E+01
1.08E+01
1.16E+01
1.22E+01
1.25E+01
1.24E+01
1.19E+01
1.17E+01
1.16E+01

8.41E-06
1.73E-03
2.48E-02
1.22E-01
3.18E-01
5.74E-01
8.45E-01
1.23E+00
1.41E+00
1.40E+00
1.26E+00
1.04E+00
8.02E-01
5.74E-01
4.78E-01
4.50E-01
4.53E-01
4.80E-01
5.57E-01
6.63E-01
8.38E-01
1.14E+00
1.38E+00
1.75E+00
2.32E+00
2.84E+00
2.89E+00
3.36E+00
3.65E+00
4.28E+00
5.14E+00
5.58E+00
5.82E+00
6.15E+00
6.29E+00
6.74E+00
7.23E+00
7.88E+00
8.64E+00
9.61E+00
1.09E+01
1.22E+01
1.34E+01
1.34E+01
1.56E+01
1.76E+01
2.08E+01
2.29E+01
2.46E+01
2.55E+01
2.64E+01

3.34E-07
1.70E-04
5.50E-03
3.95E-02
1.30E-01
2.82E-01
4.68E-01
8.09E-01
1.01E+00
1.09E+00
1.03E+00
9.07E-01
7.08E-01
5.30E-01
4.47E-01
4.28E-01
4.33E-01
4.58E-01
5.41E-01
6.43E-01
8.11E-01
1.13E+00
1.39E+00
1.75E+00
2.36E+00
2.85E+00
2.89E+00
3.35E+00
3.66E+00
4.33E+00
5.12E+00
5.57E+00
5.92E+00
6.26E+00
6.38E+00
6.83E+00
7.37E+00
8.05E+00
8.74E+00
9.32E+00
1.10E+01
1.26E+01
1.40E+01
1.43E+01
1.71E+01
1.95E+01
2.57E+01
3.09E+01
3.79E+01
4.22E+01
4.53E+01

4.34E-05
3.28E-03
3.64E-02
1.37E-01
2.94E-01
4.63E-01
6.03E-01
7.58E-01
7.91E-01
7.62E-01
6.74E-01
5.61E-01
4.48E-01
3.39E-01
2.95E-01
2.85E-01
2.94E-01
3.15E-01
3.77E-01
4.52E-01
5.80E-01
8.10E-01
1.01E+00
1.28E+00
1.75E+00
2.22E+00
2.26E+00
2.64E+00
2.90E+00
3.48E+00
4.20E+00
4.63E+00
4.87E+00
5.18E+00
5.25E+00
5.76E+00
6.20E+00
6.75E+00
7.32E+00
7.86E+00
8.63E+00
9.35E+00
9.99E+00
1.01E+01
1.14E+01
1.27E+01
1.58E+01
1.89E+01
2.45E+01
2.95E+01
3.36E+01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
2005
2006
2007
2008
2009
2010

Figure C.1.1a Conversion coefficients from photon fluence to the maximum absorbed dose in
the sensitive cells or the complete lens, for left or right irradiations (Behrens, 2017a).

FINAL DRAFT JULY 2017

2011
2012

NOT TO BE REFERENCED

Table C.1.1b Conversion coefficients from photon air kerma to the maximum absorbed dose to thesensitive cells or the complete lens, for left or right irradiations (Behrens, 2017a).
dlens, max(α)/ (Gy Gy-1) for a radiation incidence at 
Ep / MeV
0.005
0.006
0.007
0.008
0.009
0.01
0.011
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.12
0.15
0.2
0.24
0.3
0.4
0.5
0.511
0.6
0.662
0.8
1
1.117
1.2
1.3
1.33
1.5
1.7
2
2.4
3
4
5
6
6.129
8
10
15
20
30
40
50

2013

0

15

30

45

60

75

90

ROT

1.36E-06
3.64E-04
7.27E-03
3.78E-02
1.02E-01
1.91E-01
2.89E-01
4.74E-01
6.21E-01
7.36E-01
8.63E-01
9.94E-01
1.14E+00
1.35E+00
1.50E+00
1.56E+00
1.58E+00
1.57E+00
1.51E+00
1.44E+00
1.40E+00
1.32E+00
1.31E+00
1.26E+00
1.21E+00
1.19E+00
1.18E+00
1.18E+00
1.17E+00
1.15E+00
1.13E+00
1.13E+00
1.13E+00
1.10E+00
1.10E+00
1.07E+00
1.03E+00
9.32E-01
7.99E-01
6.36E-01
4.63E-01
3.62E-01
2.98E-01
2.92E-01
2.20E-01
1.73E-01
1.15E-01
8.69E-02
5.84E-02
4.39E-02
3.49E-02

2.50E-06
4.38E-04
6.90E-03
3.49E-02
9.53E-02
1.80E-01
2.78E-01
4.71E-01
6.26E-01
7.48E-01
8.82E-01
1.01E+00
1.18E+00
1.39E+00
1.53E+00
1.60E+00
1.61E+00
1.58E+00
1.51E+00
1.46E+00
1.40E+00
1.34E+00
1.32E+00
1.27E+00
1.23E+00
1.19E+00
1.19E+00
1.18E+00
1.17E+00
1.16E+00
1.13E+00
1.14E+00
1.13E+00
1.12E+00
1.12E+00
1.08E+00
1.03E+00
9.48E-01
8.10E-01
6.51E-01
4.82E-01
3.77E-01
3.12E-01
3.08E-01
2.32E-01
1.81E-01
1.21E-01
9.00E-02
6.00E-02
4.48E-02
3.62E-02

5.01E-06
4.98E-04
6.78E-03
3.20E-02
8.68E-02
1.66E-01
2.59E-01
4.47E-01
6.04E-01
7.30E-01
8.78E-01
1.01E+00
1.17E+00
1.41E+00
1.56E+00
1.62E+00
1.62E+00
1.59E+00
1.53E+00
1.46E+00
1.41E+00
1.36E+00
1.32E+00
1.28E+00
1.24E+00
1.21E+00
1.22E+00
1.20E+00
1.18E+00
1.17E+00
1.15E+00
1.14E+00
1.14E+00
1.12E+00
1.12E+00
1.09E+00
1.05E+00
9.64E-01
8.46E-01
6.93E-01
5.29E-01
4.29E-01
3.63E-01
3.50E-01
2.74E-01
2.15E-01
1.39E-01
1.01E-01
6.68E-02
5.01E-02
3.95E-02

4.95E-06
4.95E-04
6.16E-03
2.86E-02
7.63E-02
1.48E-01
2.34E-01
4.07E-01
5.60E-01
6.85E-01
8.24E-01
9.70E-01
1.13E+00
1.37E+00
1.54E+00
1.61E+00
1.61E+00
1.58E+00
1.54E+00
1.47E+00
1.41E+00
1.37E+00
1.33E+00
1.33E+00
1.26E+00
1.23E+00
1.24E+00
1.22E+00
1.21E+00
1.19E+00
1.18E+00
1.16E+00
1.16E+00
1.16E+00
1.14E+00
1.12E+00
1.08E+00
1.01E+00
9.16E-01
7.89E-01
6.32E-01
5.41E-01
4.70E-01
4.63E-01
3.71E-01
2.97E-01
1.91E-01
1.35E-01
8.51E-02
6.10E-02
4.79E-02

2.25E-06
2.76E-04
3.97E-03
2.01E-02
5.63E-02
1.15E-01
1.90E-01
3.62E-01
5.19E-01
6.51E-01
8.09E-01
9.59E-01
1.15E+00
1.38E+00
1.53E+00
1.60E+00
1.60E+00
1.60E+00
1.54E+00
1.46E+00
1.41E+00
1.34E+00
1.32E+00
1.29E+00
1.25E+00
1.24E+00
1.24E+00
1.22E+00
1.20E+00
1.20E+00
1.17E+00
1.15E+00
1.15E+00
1.15E+00
1.15E+00
1.12E+00
1.10E+00
1.05E+00
9.89E-01
9.02E-01
7.94E-01
7.15E-01
6.62E-01
6.55E-01
5.74E-01
5.06E-01
3.62E-01
2.74E-01
1.74E-01
1.26E-01
9.77E-02

2.74E-07
8.16E-05
1.60E-03
1.03E-02
3.45E-02
7.75E-02
1.40E-01
2.91E-01
4.51E-01
5.86E-01
7.51E-01
9.05E-01
1.11E+00
1.34E+00
1.48E+00
1.56E+00
1.58E+00
1.57E+00
1.50E+00
1.44E+00
1.40E+00
1.33E+00
1.30E+00
1.26E+00
1.22E+00
1.19E+00
1.19E+00
1.18E+00
1.17E+00
1.15E+00
1.15E+00
1.14E+00
1.13E+00
1.12E+00
1.12E+00
1.10E+00
1.08E+00
1.04E+00
1.01E+00
9.63E-01
9.01E-01
8.61E-01
8.30E-01
8.13E-01
7.73E-01
7.28E-01
6.04E-01
5.04E-01
3.59E-01
2.73E-01
2.21E-01

1.09E-08
7.99E-06
3.55E-04
3.35E-03
1.41E-02
3.82E-02
7.74E-02
1.91E-01
3.24E-01
4.56E-01
6.15E-01
7.89E-01
9.81E-01
1.24E+00
1.38E+00
1.48E+00
1.51E+00
1.49E+00
1.46E+00
1.40E+00
1.35E+00
1.32E+00
1.31E+00
1.26E+00
1.25E+00
1.20E+00
1.19E+00
1.18E+00
1.18E+00
1.17E+00
1.14E+00
1.14E+00
1.15E+00
1.14E+00
1.14E+00
1.11E+00
1.10E+00
1.07E+00
1.02E+00
9.35E-01
9.04E-01
8.89E-01
8.68E-01
8.69E-01
8.47E-01
8.07E-01
7.47E-01
6.81E-01
5.53E-01
4.52E-01
3.80E-01

1.42E-06
1.54E-04
2.35E-03
1.16E-02
3.19E-02
6.25E-02
9.97E-02
1.79E-01
2.53E-01
3.19E-01
4.00E-01
4.87E-01
6.21E-01
7.91E-01
9.15E-01
9.86E-01
1.02E+00
1.03E+00
1.01E+00
9.82E-01
9.67E-01
9.46E-01
9.55E-01
9.28E-01
9.27E-01
9.31E-01
9.28E-01
9.28E-01
9.31E-01
9.41E-01
9.36E-01
9.48E-01
9.42E-01
9.43E-01
9.39E-01
9.37E-01
9.22E-01
8.93E-01
8.54E-01
7.88E-01
7.11E-01
6.60E-01
6.18E-01
6.15E-01
5.67E-01
5.26E-01
4.59E-01
4.17E-01
3.57E-01
3.16E-01
2.82E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2014
2015
2016
2017
2018
2019
2020
2021
2022
2023
2024
2025
2026
2027
2028
2029
2030
2031
2032

Figure C.1.1b Conversion coefficients from photon air kerma to the maximum absorbed dose in
the sensitive cells or the complete lens, for left or right irradiations (Behrens, 2017a).

FINAL DRAFT JULY 2017

2033
2034
2035
2036
2037

Table C.1.2 Neutrons
Figure C.1.2 Neutrons

NOT TO BE REFERENCED

FINAL DRAFT JULY 2017

2038
2039

NOT TO BE REFERENCED

Table C.1.3 Conversion coefficients from electron fluence to the maximum absorbed dose in thesensitive cells or the complete lens, for left or right irradiations (Behrens,2017a).
dlens, max (α )/ (pGy cm2) for a radiation incidence at 
Ep / MeV
0.01
0.015
0.02
0.03
0.04
0.05
0.06
0.08
0.1
0.15
0.2
0.3
0.4
0.5
0.6
0.7
0.8
1
1.25
1.5
1.75
2
2.5
3
3.5
4
5
6
7
8
10
15
20
30
40
50

2040

0

15

30

45

60

75

90

ROT

1.68E-06
2.26E-05
8.15E-05
2.23E-04
4.16E-04
6.07E-04
8.47E-04
1.31E-03
1.92E-03
3.24E-03
5.04E-03
9.58E-03
1.41E-02
2.06E-02
1.75E-01
7.56E+00
4.62E+01
2.29E+02
3.87E+02
4.42E+02
4.45E+02
4.30E+02
4.08E+02
3.78E+02
3.54E+02
3.39E+02
3.23E+02
3.15E+02
3.10E+02
3.07E+02
3.04E+02
3.01E+02
3.01E+02
3.03E+02
3.03E+02
3.00E+02

1.81E-06
3.34E-05
7.79E-05
2.30E-04
3.40E-04
6.75E-04
8.68E-04
1.33E-03
1.80E-03
3.36E-03
5.21E-03
9.08E-03
1.47E-02
2.06E-02
2.32E-01
8.46E+00
4.66E+01
2.18E+02
3.73E+02
4.30E+02
4.41E+02
4.29E+02
4.12E+02
3.87E+02
3.66E+02
3.51E+02
3.35E+02
3.28E+02
3.22E+02
3.18E+02
3.12E+02
3.06E+02
3.03E+02
3.04E+02
3.07E+02
3.01E+02

1.43E-06
2.34E-05
7.25E-05
2.25E-04
4.04E-04
6.16E-04
7.80E-04
1.23E-03
1.66E-03
3.11E-03
4.60E-03
7.91E-03
1.29E-02
1.91E-02
3.17E-01
9.60E+00
4.57E+01
1.89E+02
3.29E+02
3.94E+02
4.17E+02
4.19E+02
4.13E+02
3.99E+02
3.82E+02
3.69E+02
3.54E+02
3.49E+02
3.46E+02
3.41E+02
3.30E+02
3.09E+02
3.05E+02
3.06E+02
3.03E+02
3.06E+02

1.16E-06
2.22E-05
5.81E-05
1.89E-04
3.49E-04
5.09E-04
6.15E-04
1.08E-03
1.57E-03
2.47E-03
4.07E-03
7.83E-03
1.25E-02
1.76E-02
2.97E-01
8.88E+00
3.93E+01
1.50E+02
2.69E+02
3.39E+02
3.80E+02
4.01E+02
4.09E+02
4.11E+02
4.05E+02
3.99E+02
3.92E+02
3.94E+02
4.01E+02
4.06E+02
4.03E+02
3.53E+02
3.23E+02
3.12E+02
3.13E+02
3.10E+02

7.55E-07
1.96E-05
4.99E-05
1.26E-04
2.71E-04
4.08E-04
5.57E-04
8.32E-04
1.20E-03
2.23E-03
3.47E-03
6.02E-03
1.00E-02
1.41E-02
1.86E-01
6.08E+00
2.77E+01
1.04E+02
1.92E+02
2.57E+02
3.06E+02
3.39E+02
3.75E+02
3.85E+02
3.91E+02
3.87E+02
3.68E+02
3.49E+02
3.37E+02
3.56E+02
4.20E+02
4.60E+02
4.28E+02
3.71E+02
3.47E+02
3.41E+02

7.04E-07
1.66E-05
3.24E-05
1.12E-04
2.00E-04
3.06E-04
3.87E-04
6.11E-04
7.97E-04
1.65E-03
2.59E-03
4.52E-03
7.88E-03
1.13E-02
7.49E-02
2.89E+00
1.50E+01
6.11E+01
1.19E+02
1.69E+02
2.12E+02
2.52E+02
3.13E+02
3.49E+02
3.70E+02
3.80E+02
3.82E+02
3.76E+02
3.64E+02
3.53E+02
3.36E+02
3.15E+02
3.76E+02
3.67E+02
3.46E+02
3.32E+02

3.74E-07
6.43E-06
2.73E-05
6.60E-05
1.02E-04
1.86E-04
2.24E-04
4.21E-04
5.48E-04
1.02E-03
1.64E-03
3.11E-03
5.09E-03
7.66E-03
2.32E-02
8.98E-01
5.51E+00
2.66E+01
5.77E+01
8.67E+01
1.16E+02
1.46E+02
2.02E+02
2.46E+02
2.85E+02
3.14E+02
3.50E+02
3.69E+02
3.75E+02
3.76E+02
3.61E+02
3.29E+02
3.15E+02
3.20E+02
3.20E+02
3.21E+02

3.32E-07
4.60E-06
3.40E-05
7.02E-05
1.13E-04
1.72E-04
2.83E-04
4.60E-04
5.86E-04
1.20E-03
1.77E-03
3.20E-03
4.83E-03
7.78E-03
9.44E-02
3.08E+00
1.54E+01
6.64E+01
1.17E+02
1.44E+02
1.57E+02
1.62E+02
1.65E+02
1.64E+02
1.64E+02
1.64E+02
1.65E+02
1.68E+02
1.72E+02
1.77E+02
1.85E+02
2.01E+02
2.12E+02
2.36E+02
2.64E+02
2.90E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2041
2042
2043
2044
2045
2046
2047
2048
2049
2050
2051
2052
2053
2054
2055
2056
2057
2058
2059
2060
2061
2062

Figure C.1.3 Conversion coefficients from electron fluence to the maximum absorbed dose in thesensitive cells or the complete lens, for left or right irradiations (Behrens, 2017a).

FINAL DRAFT JULY 2017

2063
2064

NOT TO BE REFERENCED

Table C.1.4 Conversion coefficients from positron fluence to the maximum absorbed dose in thesensitive cells or the complete lens, for left or right irradiations (Behrens, 2017a).
dlens, max (α )/ (pGy cm2) for a radiation incidence at 
Ep / MeV
0.001
0.002
0.003
0.004
0.005
0.006
0.007
0.008
0.009
0.01
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.15
0.2
0.3
0.4
0.5
0.6
0.7
0.8
1
1.25
1.5
1.75
2
2.5
3
3.5
4
5
6
7
8
10
15
20
30
40
50

2065

0

15

30

45

60

75

90

ROT

7.43E+00
7.17E+00
6.99E+00
6.88E+00
7.02E+00
6.97E+00
6.85E+00
6.92E+00
6.84E+00
6.87E+00
6.78E+00
6.88E+00
6.96E+00
6.79E+00
6.93E+00
6.95E+00
6.94E+00
6.87E+00
6.91E+00
6.99E+00
6.96E+00
6.97E+00
6.94E+00
7.13E+00
7.29E+00
7.60E+00
7.91E+00
8.44E+00
1.71E+01
5.95E+01
2.48E+02
3.94E+02
4.34E+02
4.32E+02
4.13E+02
3.88E+02
3.59E+02
3.38E+02
3.22E+02
3.10E+02
3.05E+02
3.00E+02
2.99E+02
2.96E+02
2.97E+02
2.98E+02
2.99E+02
2.99E+02
3.02E+02

7.94E+00
7.47E+00
7.26E+00
7.34E+00
7.17E+00
7.18E+00
7.31E+00
7.31E+00
7.30E+00
7.26E+00
7.32E+00
7.29E+00
7.19E+00
7.13E+00
7.22E+00
7.18E+00
7.15E+00
7.20E+00
7.04E+00
7.17E+00
7.20E+00
7.43E+00
7.30E+00
7.42E+00
7.61E+00
7.97E+00
8.35E+00
8.70E+00
1.84E+01
5.97E+01
2.37E+02
3.79E+02
4.24E+02
4.24E+02
4.13E+02
3.94E+02
3.69E+02
3.47E+02
3.36E+02
3.22E+02
3.17E+02
3.12E+02
3.06E+02
3.02E+02
3.01E+02
2.99E+02
2.99E+02
3.03E+02
3.00E+02

7.89E+00
7.43E+00
7.39E+00
7.28E+00
7.29E+00
7.33E+00
7.22E+00
7.21E+00
7.14E+00
7.18E+00
7.20E+00
7.08E+00
7.23E+00
7.17E+00
7.28E+00
7.27E+00
7.26E+00
7.20E+00
7.28E+00
7.35E+00
7.21E+00
7.26E+00
7.30E+00
7.60E+00
7.66E+00
7.71E+00
8.11E+00
8.86E+00
1.95E+01
5.86E+01
2.06E+02
3.35E+02
3.90E+02
4.10E+02
4.05E+02
3.97E+02
3.78E+02
3.65E+02
3.53E+02
3.42E+02
3.38E+02
3.34E+02
3.32E+02
3.23E+02
3.06E+02
3.01E+02
3.00E+02
3.03E+02
3.03E+02

7.35E+00
6.98E+00
6.71E+00
6.64E+00
6.72E+00
6.59E+00
6.65E+00
6.65E+00
6.60E+00
6.61E+00
6.62E+00
6.55E+00
6.56E+00
6.59E+00
6.57E+00
6.49E+00
6.69E+00
6.76E+00
6.74E+00
6.48E+00
6.80E+00
6.71E+00
6.68E+00
6.93E+00
6.97E+00
7.12E+00
7.36E+00
8.11E+00
1.80E+01
5.03E+01
1.64E+02
2.77E+02
3.41E+02
3.72E+02
3.87E+02
3.92E+02
3.96E+02
3.85E+02
3.81E+02
3.74E+02
3.80E+02
3.84E+02
3.91E+02
3.88E+02
3.40E+02
3.16E+02
3.07E+02
3.03E+02
3.02E+02

6.13E+00
5.88E+00
5.61E+00
5.70E+00
5.67E+00
5.54E+00
5.58E+00
5.51E+00
5.57E+00
5.52E+00
5.53E+00
5.65E+00
5.55E+00
5.49E+00
5.59E+00
5.59E+00
5.62E+00
5.55E+00
5.61E+00
5.52E+00
5.61E+00
5.57E+00
5.63E+00
5.76E+00
5.80E+00
5.88E+00
6.23E+00
6.67E+00
1.34E+01
3.65E+01
1.15E+02
2.03E+02
2.61E+02
3.06E+02
3.35E+02
3.68E+02
3.69E+02
3.73E+02
3.68E+02
3.49E+02
3.36E+02
3.25E+02
3.46E+02
4.08E+02
4.39E+02
4.12E+02
3.59E+02
3.40E+02
3.31E+02

4.91E+00
4.58E+00
4.43E+00
4.36E+00
4.24E+00
4.33E+00
4.33E+00
4.27E+00
4.30E+00
4.31E+00
4.23E+00
4.38E+00
4.30E+00
4.24E+00
4.30E+00
4.31E+00
4.39E+00
4.29E+00
4.31E+00
4.33E+00
4.38E+00
4.25E+00
4.23E+00
4.43E+00
4.50E+00
4.70E+00
4.70E+00
4.98E+00
8.33E+00
2.15E+01
6.88E+01
1.27E+02
1.72E+02
2.13E+02
2.50E+02
3.04E+02
3.37E+02
3.53E+02
3.69E+02
3.70E+02
3.60E+02
3.46E+02
3.38E+02
3.23E+02
3.10E+02
3.58E+02
3.47E+02
3.30E+02
3.23E+02

3.47E+00
3.21E+00
3.05E+00
3.01E+00
3.07E+00
2.91E+00
2.98E+00
2.95E+00
2.94E+00
2.94E+00
2.98E+00
2.92E+00
2.94E+00
3.01E+00
2.92E+00
2.94E+00
2.91E+00
2.92E+00
3.00E+00
2.96E+00
3.01E+00
3.00E+00
2.98E+00
2.99E+00
3.12E+00
3.16E+00
3.24E+00
3.39E+00
4.46E+00
9.54E+00
3.18E+01
6.18E+01
9.22E+01
1.20E+02
1.46E+02
2.03E+02
2.47E+02
2.76E+02
3.03E+02
3.40E+02
3.52E+02
3.64E+02
3.61E+02
3.44E+02
3.23E+02
3.11E+02
3.09E+02
3.06E+02
3.10E+02

3.06E+00
2.87E+00
2.76E+00
2.72E+00
2.74E+00
2.70E+00
2.69E+00
2.77E+00
2.73E+00
2.67E+00
2.65E+00
2.69E+00
2.63E+00
2.72E+00
2.67E+00
2.68E+00
2.67E+00
2.77E+00
2.71E+00
2.68E+00
2.71E+00
2.73E+00
2.79E+00
2.75E+00
2.90E+00
2.96E+00
3.02E+00
3.26E+00
6.91E+00
2.02E+01
7.28E+01
1.21E+02
1.45E+02
1.54E+02
1.58E+02
1.59E+02
1.61E+02
1.59E+02
1.58E+02
1.60E+02
1.63E+02
1.69E+02
1.71E+02
1.80E+02
1.94E+02
2.07E+02
2.31E+02
2.60E+02
2.83E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2066
2067
2068
2069
2070
2071
2072
2073
2074
2075
2076
2077
2078
2079
2080
2081
2082
2083
2084
2085

Figure C.1.4 Conversion coefficients from positron fluence to the maximum absorbed dose in
the sensitive cells or the complete lens, for left or right irradiations (Behrens, 2017a).

FINAL DRAFT JULY 20172086

NOT TO BE REFERENCED

C.2 Photons for Energies up to 50MeV in Fields with Charged-Particle Equilibrium.

2087

The calibration of are monitoring instruments and personal dosimeters to measure photons for

2088

ambient dose, directional and personal absorbed dose in the lens of the eye and local skin, and personal2089

dose, are performed routinely in air with sufficient material in front of the instrument to provide full2090

charged-particle equilibrium. The calibration procedure is for photons and for the particles produced in

2091

air and the other material at the point of test.

2092

Table C.2.1a and Figure C.2.1a give values of conversion coefficients for this procedure for2093

photon energies up to 50 MeV using the kerma-approximation method to give charged-particle

2094

equilibrium, from photon fluence to directional and personal absorbed dose in the lens of the eye, and in

2095

Table C.2.1b and Figure C.2.1b from air kerma. The conversion coefficients are to the value of the2096

absorbed dose to the lens of the eye, the maximum value of that to the radiation sensitive cells or the2097

complete lens, calculated for whole-body exposure of the stylized eye model (Behrens and Dietze, 2011)2098

for broad parallel beams incident for angles from 0° (A-P) to 90° in 15° steps, the maximum value of2099

the absorbed dose of the right or left irradiations is taken; and for a rotational field.

2100
2101

FINAL DRAFT JULY 2017

2102
2103
2104

NOT TO BE REFERENCED

Table C.2.1a Conversion coefficients from photon fluence to the maximum absorbed dose in thesensitive cells or the complete lens, for left or right irradiations, calculated using the kermaapproximation method (Behrens, 2017a).
dlens, max(α )/ (pGy cm2) for a radiation incidence at 

Ep / MeV
0.005
0.006
0.007
0.008
0.009
0.01
0.011
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.12
0.15
0.2
0.24
0.3
0.4
0.5
0.511
0.6
0.662
0.8
1
1.117
1.2
1.3
1.33
1.5
1.7
2
2.4
3
4
5
6
6.129
8
10
15
20
30
40
50

0

15

30

45

60

75

90

ROT

4.10E-05
7.94E-03
1.07E-01
4.25E-01
9.03E-01
1.38E+00
1.73E+00
2.02E+00
1.98E+00
1.80E+00
1.49E+00
1.16E+00
8.53E-01
5.89E-01
4.89E-01
4.55E-01
4.56E-01
4.81E-01
5.59E-01
6.64E-01
8.35E-01
1.14E+00
1.38E+00
1.75E+00
2.30E+00
2.82E+00
2.91E+00
3.35E+00
3.64E+00
4.24E+00
5.09E+00
5.58E+00
5.83E+00
6.23E+00
6.32E+00
6.89E+00
7.49E+00
8.39E+00
9.44E+00
1.10E+01
1.32E+01
1.54E+01
1.74E+01
1.76E+01
2.15E+01
2.54E+01
3.59E+01
4.63E+01
6.96E+01
9.40E+01
1.19E+02

6.91E-05
8.87E-03
1.06E-01
4.12E-01
8.76E-01
1.34E+00
1.69E+00
2.00E+00
1.96E+00
1.79E+00
1.49E+00
1.17E+00
8.48E-01
5.95E-01
4.90E-01
4.56E-01
4.63E-01
4.87E-01
5.62E-01
6.70E-01
8.39E-01
1.14E+00
1.40E+00
1.76E+00
2.37E+00
2.85E+00
2.91E+00
3.37E+00
3.65E+00
4.33E+00
5.10E+00
5.57E+00
5.93E+00
6.27E+00
6.36E+00
6.98E+00
7.58E+00
8.44E+00
9.53E+00
1.10E+01
1.33E+01
1.54E+01
1.74E+01
1.77E+01
2.17E+01
2.55E+01
3.61E+01
4.66E+01
6.97E+01
9.35E+01
1.19E+02

1.48E-04
1.06E-02
1.05E-01
3.79E-01
7.97E-01
1.23E+00
1.57E+00
1.90E+00
1.89E+00
1.74E+00
1.47E+00
1.15E+00
8.50E-01
5.97E-01
4.98E-01
4.64E-01
4.66E-01
4.91E-01
5.72E-01
6.73E-01
8.48E-01
1.16E+00
1.40E+00
1.76E+00
2.34E+00
2.88E+00
2.95E+00
3.42E+00
3.69E+00
4.31E+00
5.15E+00
5.71E+00
5.94E+00
6.29E+00
6.37E+00
6.92E+00
7.59E+00
8.47E+00
9.52E+00
1.11E+01
1.34E+01
1.55E+01
1.75E+01
1.77E+01
2.15E+01
2.57E+01
3.57E+01
4.69E+01
6.96E+01
9.35E+01
1.20E+02

1.56E-04
1.02E-02
9.16E-02
3.24E-01
6.77E-01
1.06E+00
1.39E+00
1.74E+00
1.77E+00
1.67E+00
1.43E+00
1.14E+00
8.50E-01
5.96E-01
5.00E-01
4.67E-01
4.67E-01
4.90E-01
5.71E-01
6.74E-01
8.50E-01
1.17E+00
1.41E+00
1.79E+00
2.37E+00
2.93E+00
3.00E+00
3.48E+00
3.78E+00
4.39E+00
5.25E+00
5.69E+00
5.99E+00
6.41E+00
6.46E+00
7.04E+00
7.68E+00
8.56E+00
9.71E+00
1.11E+01
1.33E+01
1.57E+01
1.76E+01
1.80E+01
2.15E+01
2.55E+01
3.57E+01
4.66E+01
6.93E+01
9.40E+01
1.19E+02

5.95E-05
5.73E-03
6.22E-02
2.35E-01
5.21E-01
8.58E-01
1.15E+00
1.53E+00
1.63E+00
1.55E+00
1.35E+00
1.11E+00
8.24E-01
5.90E-01
4.97E-01
4.62E-01
4.64E-01
4.88E-01
5.65E-01
6.72E-01
8.45E-01
1.15E+00
1.42E+00
1.80E+00
2.39E+00
3.01E+00
2.98E+00
3.49E+00
3.78E+00
4.41E+00
5.31E+00
5.74E+00
6.03E+00
6.43E+00
6.51E+00
7.10E+00
7.78E+00
8.62E+00
9.72E+00
1.12E+01
1.34E+01
1.56E+01
1.75E+01
1.81E+01
2.16E+01
2.55E+01
3.59E+01
4.67E+01
6.94E+01
9.49E+01
1.19E+02

7.94E-06
1.56E-03
2.67E-02
1.23E-01
3.20E-01
5.79E-01
8.45E-01
1.25E+00
1.41E+00
1.40E+00
1.26E+00
1.05E+00
7.93E-01
5.77E-01
4.80E-01
4.46E-01
4.52E-01
4.78E-01
5.59E-01
6.66E-01
8.39E-01
1.15E+00
1.40E+00
1.76E+00
2.34E+00
2.86E+00
2.90E+00
3.39E+00
3.66E+00
4.32E+00
5.13E+00
5.57E+00
5.90E+00
6.25E+00
6.37E+00
6.90E+00
7.55E+00
8.42E+00
9.48E+00
1.10E+01
1.32E+01
1.53E+01
1.74E+01
1.76E+01
2.15E+01
2.56E+01
3.55E+01
4.65E+01
7.00E+01
9.33E+01
1.18E+02

4.11E-07
1.74E-04
4.67E-03
3.65E-02
1.22E-01
2.63E-01
4.43E-01
7.87E-01
1.02E+00
1.11E+00
1.07E+00
9.27E-01
7.28E-01
5.35E-01
4.53E-01
4.28E-01
4.34E-01
4.60E-01
5.42E-01
6.44E-01
8.19E-01
1.13E+00
1.38E+00
1.73E+00
2.29E+00
2.85E+00
2.92E+00
3.38E+00
3.65E+00
4.31E+00
5.12E+00
5.56E+00
5.88E+00
6.26E+00
6.35E+00
6.90E+00
7.54E+00
8.37E+00
9.60E+00
1.09E+01
1.32E+01
1.55E+01
1.75E+01
1.76E+01
2.16E+01
2.56E+01
3.56E+01
4.64E+01
6.86E+01
9.23E+01
1.18E+02

3.06E-05
3.13E-03
3.39E-02
1.29E-01
2.85E-01
4.52E-01
5.92E-01
7.59E-01
7.97E-01
7.72E-01
6.87E-01
5.79E-01
4.59E-01
3.43E-01
2.99E-01
2.86E-01
2.95E-01
3.15E-01
3.77E-01
4.56E-01
5.81E-01
8.17E-01
1.00E+00
1.30E+00
1.75E+00
2.23E+00
2.26E+00
2.64E+00
2.92E+00
3.46E+00
4.24E+00
4.63E+00
4.92E+00
5.25E+00
5.39E+00
5.98E+00
6.49E+00
7.25E+00
8.33E+00
9.82E+00
1.19E+01
1.39E+01
1.59E+01
1.61E+01
1.94E+01
2.36E+01
3.32E+01
4.35E+01
6.45E+01
8.72E+01
1.09E+02

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2105
2106
2107
2108
2109
2110
2111
2112
2113
2114
2115
2116
2117
2118
2119
2120
2121
2122
2123
2124
2125

Figure C.2.1a Conversion coefficients from photon fluence to the maximum absorbed dose in thesensitive cells or the complete lens, for left or right irradiations, calculated using the kermaapproximation method (Behrens, 2017a).

FINAL DRAFT JULY 2017

2126
2127
2128

NOT TO BE REFERENCED

Table C.2.1b Conversion coefficients from photon air kerma to the maximum absorbed dose in thesensitive cells or the complete lens, for left or right irradiations, calculated using the kermaapproximation method (Behrens, 2017a).
dlens, max(α)/(Gy Gy-1) for a radiation incidence at 

Ep / MeV
0.005
0.006
0.007
0.008
0.009
0.01
0.011
0.013
0.015
0.017
0.02
0.024
0.03
0.04
0.05
0.06
0.07
0.08
0.1
0.12
0.15
0.2
0.24
0.3
0.4
0.5
0.511
0.6
0.662
0.8
1
1.117
1.2
1.3
1.33
1.5
1.7
2
2.4
3
4
5
6
6.129
8
10
15
20
30
40
50

0
1.34E-06
3.74E-04
6.88E-03
3.61E-02
9.80E-02
1.86E-01
2.86E-01
4.78E-01
6.33E-01
7.56E-01
8.87E-01
1.01E+00
1.18E+00
1.37E+00
1.52E+00
1.57E+00
1.58E+00
1.57E+00
1.51E+00
1.44E+00
1.39E+00
1.33E+00
1.30E+00
1.27E+00
1.22E+00
1.19E+00
1.20E+00
1.18E+00
1.17E+00
1.15E+00
1.14E+00
1.14E+00
1.13E+00
1.13E+00
1.13E+00
1.12E+00
1.11E+00
1.11E+00
1.10E+00
1.10E+00
1.09E+00
1.09E+00
1.08E+00
1.07E+00
1.07E+00
1.05E+00
1.04E+00
1.02E+00
1.01E+00
1.01E+00
9.95E-0115
2.25E-06
4.17E-04
6.86E-03
3.50E-02
9.50E-02
1.81E-01
2.79E-01
4.71E-01
6.26E-01
7.49E-01
8.83E-01
1.02E+00
1.18E+00
1.39E+00
1.52E+00
1.58E+00
1.61E+00
1.59E+00
1.51E+00
1.45E+00
1.40E+00
1.34E+00
1.32E+00
1.27E+00
1.25E+00
1.20E+00
1.20E+00
1.18E+00
1.17E+00
1.17E+00
1.14E+00
1.14E+00
1.15E+00
1.14E+00
1.14E+00
1.13E+00
1.13E+00
1.12E+00
1.11E+00
1.11E+00
1.10E+00
1.08E+00
1.08E+00
1.08E+00
1.08E+00
1.05E+00
1.05E+00
1.03E+00
1.02E+00
1.00E+00
1.00E+0030
4.84E-06
4.99E-04
6.75E-03
3.21E-02
8.65E-02
1.66E-01
2.59E-01
4.48E-01
6.03E-01
7.29E-01
8.74E-01
1.00E+00
1.18E+00
1.39E+00
1.54E+00
1.61E+00
1.62E+00
1.60E+00
1.54E+00
1.46E+00
1.42E+00
1.35E+00
1.32E+00
1.27E+00
1.24E+00
1.21E+00
1.21E+00
1.20E+00
1.19E+00
1.16E+00
1.15E+00
1.17E+00
1.15E+00
1.14E+00
1.14E+00
1.13E+00
1.13E+00
1.12E+00
1.11E+00
1.11E+00
1.11E+00
1.09E+00
1.08E+00
1.07E+00
1.07E+00
1.07E+00
1.03E+00
1.03E+00
1.01E+00
1.00E+00
1.01E+00

45
5.10E-06
4.79E-04
5.91E-03
2.75E-02
7.35E-02
1.44E-01
2.29E-01
4.11E-01
5.68E-01
7.01E-01
8.47E-01
9.90E-01
1.18E+00
1.39E+00
1.55E+00
1.61E+00
1.62E+00
1.60E+00
1.54E+00
1.46E+00
1.42E+00
1.36E+00
1.33E+00
1.29E+00
1.25E+00
1.23E+00
1.23E+00
1.22E+00
1.21E+00
1.19E+00
1.17E+00
1.16E+00
1.16E+00
1.17E+00
1.15E+00
1.15E+00
1.14E+00
1.13E+00
1.13E+00
1.11E+00
1.10E+00
1.11E+00
1.09E+00
1.09E+00
1.07E+00
1.06E+00
1.04E+00
1.03E+00
1.01E+00
1.01E+00
9.97E-0160
1.94E-06
2.69E-04
4.01E-03
1.99E-02
5.65E-02
1.16E-01
1.90E-01
3.61E-01
5.22E-01
6.49E-01
8.03E-01
9.62E-01
1.14E+00
1.38E+00
1.54E+00
1.60E+00
1.61E+00
1.59E+00
1.52E+00
1.46E+00
1.41E+00
1.34E+00
1.34E+00
1.30E+00
1.26E+00
1.26E+00
1.22E+00
1.23E+00
1.22E+00
1.19E+00
1.18E+00
1.18E+00
1.17E+00
1.17E+00
1.16E+00
1.15E+00
1.16E+00
1.14E+00
1.14E+00
1.13E+00
1.10E+00
1.10E+00
1.08E+00
1.10E+00
1.07E+00
1.06E+00
1.04E+00
1.03E+00
1.01E+00
1.02E+00
9.95E-0175
2.59E-07
7.33E-05
1.72E-03
1.05E-02
3.47E-02
7.82E-02
1.40E-01
2.96E-01
4.51E-01
5.86E-01
7.51E-01
9.13E-01
1.10E+00
1.34E+00
1.49E+00
1.54E+00
1.57E+00
1.56E+00
1.50E+00
1.45E+00
1.40E+00
1.34E+00
1.32E+00
1.27E+00
1.24E+00
1.20E+00
1.19E+00
1.19E+00
1.18E+00
1.17E+00
1.14E+00
1.14E+00
1.14E+00
1.14E+00
1.14E+00
1.12E+00
1.12E+00
1.11E+00
1.11E+00
1.10E+00
1.09E+00
1.08E+00
1.08E+00
1.07E+00
1.07E+00
1.06E+00
1.03E+00
1.03E+00
1.02E+00
1.00E+00
9.91E-0190
1.34E-08
8.20E-06
3.01E-04
3.09E-03
1.33E-02
3.55E-02
7.32E-02
1.86E-01
3.25E-01
4.63E-01
6.36E-01
8.07E-01
1.01E+00
1.25E+00
1.40E+00
1.48E+00
1.51E+00
1.50E+00
1.46E+00
1.40E+00
1.37E+00
1.31E+00
1.30E+00
1.25E+00
1.21E+00
1.20E+00
1.20E+00
1.19E+00
1.17E+00
1.16E+00
1.14E+00
1.14E+00
1.14E+00
1.14E+00
1.13E+00
1.12E+00
1.12E+00
1.11E+00
1.12E+00
1.09E+00
1.09E+00
1.09E+00
1.08E+00
1.07E+00
1.07E+00
1.06E+00
1.03E+00
1.02E+00
1.00E+00
9.89E-01
9.88E-01

ROT
9.99E-07
1.47E-04
2.19E-03
1.10E-02
3.09E-02
6.11E-02
9.80E-02
1.79E-01
2.55E-01
3.23E-01
4.08E-01
5.04E-01
6.35E-01
7.99E-01
9.27E-01
9.89E-01
1.03E+00
1.03E+00
1.01E+00
9.90E-01
9.69E-01
9.54E-01
9.41E-01
9.38E-01
9.27E-01
9.37E-01
9.29E-01
9.30E-01
9.37E-01
9.35E-01
9.45E-01
9.48E-01
9.52E-01
9.55E-01
9.62E-01
9.72E-01
9.65E-01
9.60E-01
9.73E-01
9.84E-01
9.77E-01
9.80E-01
9.80E-01
9.79E-01
9.66E-01
9.78E-01
9.62E-01
9.58E-01
9.41E-01
9.35E-01
9.18E-01

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2129
2130
2131
2132
2133
2134
2135
2136
2137
2138
2139
2140
2141
2142
2143
2144
2145
2146
2147
2148
2149

Figure C.2.1b Conversion coefficients from photon air kerma to the maximum absorbed dose in
the sensitive cells or the complete lens, for left or right irradiations, calculated using the kermaapproximation method (Behrens, 2017a).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2150
2151

References

2152
2153
2154
2155
2156
2157
2158
2159
2160
2161
2162
2163
2164
2165
2166
2167
2168
2169
2170
2171
2172
2173
2174
2175
2176
2177
2178
2179
2180
2181
2182
2183
2184
2185
2186
2187
2188
2189
2190

ARMSTRONG, T.W., AND CHANDLER, K.C. SPAR, a FORTRAN Program for Computing Stopping Powers
and Ranges for Muons, Charged Pions, Protons and Heavy Ions. ORNL-4869 (Oak Ridge National
Laboratory, Tennessee, TN) (1973).

2191
2192
2193

Boudard, A., Cugnon, J., David, J.C., Leray, S., and Mancusi, D. New potentialities of the Liege
intranuclear cascade model for reactions induced by nucleons and light charged particles, Phys.
Rev. C87, 014606 (2013).

2194
2195

Briesmeister, J.F. MCNP – A General Monte Carlo N-Particle Transport Code, Version 4C. Report LA13709-M (Los Alamos National Laboratory, Los Alamos, NM) (2000).

Attix, F. H. (1979a). “The partition of kerma to account for bremsstrahlung,” Health Phys. 36, 347-354.
Attix, F. H. (1979b). “Addendum to ‘The partition of kerma to account for bremsstrahlung’,” HealthPhys. 36, 536.
Ballarini, F., Battistoni, G., Cerutti, F., Empl, A., Fassò, A., Ferrari, A., Gadioli, E., Garzelli, M.V.
Ottolenghi, A., Pinsky, L.S., Ranft, J., Roesler, S., Sala, P.R. and Smirnov, G. Nuclear Models in
FLUKA: Present Capabilities, Open Problems and Future Improvements. SLAC-PUB-10813.
(SLAC, Stanford, CA.). (2004).
Bartlett, D.T. and Dietze, G. ICRU Operational Quantities. Radiat. Prot. Dosim. 139(4), 425-426(2010).
Bartlett, D.T., Dietze, G., Hertel, N., Bordy, J-M., Endo, A., Gualdrini, G., Pelliccioni, M., Ambrosi, P.,
Siebert, B. and Veinot, K. Operational Quantities for External Radiation Exposure: Deficiencies andOptions. In: the Fifth International MELODI Workshop, Brussels, 7-10 October 2013.
Behrens and Dietze Dose conversion coefficients for photon exposure of the human eye lens. Phys. Med.
Biol.56, 415-437 (2011).
Behrens, R. On the operational quantity Hp(3) for eye lens dosimetry. J. Radiol. Prot. 32, 455-464(2012).
Behrens, R. Compilation of conversion coefficients for the dose to the lens of the eye. Radiat.Prot.
Dosim. 174, 348-370 (2017a).
Behrens, R. Conversion coefficients for H'(3;Ω) for photons. J. Radiol. Prot. 37 354–378 (2017b)
Berger, M.J. Monte Carlo calculation of the penetration and diﬀusion of fast charged particles. In: Alder,
B., Fernbach, S., Rotenberg, M. (Eds.), Methods in Computational Physics. Academic Press, New
York, pp. 135–215 (1963).
Böhlen, T.T., Cerutti, F., Chin, M.P.W., A. Fassò, A., Ferrari, A., Ortega, P.G., Mairani, A., Sala, P.R.,
Smirnov, G., and Vlachoudis, V. The FLUKA code: Developments and challenges for high energy
and medical applications, Nucl. Data Sheets 120, 211-214 (2014).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2196
2197

Burlin, T.E. and Wheatley, B.M., A unified Approach to Dosimetry in Radiological Protection, Phys.
Med. Biol. 16, 47-56 (1971).

2198
2199

Burlin, T.E., Davies, M.L. and Wheatley, B.M., Cavity Ionisation Theory applied to the Design of a
Maximum Permissible Fluence Instrument, Phys. Med. Biol. 24 (1) 44-56 (1979).

2200
2201
2202

Burlin, T E, The Relevance of Fluence Data to Radiation Protection IN Proc. European Seminar on
Radiation Protection Quantities for External Exposure, Braunschweig, 1980. (Harwood/CEC:
Brussels and Luxembourg) (1981).

2203
2204
2205

Commission of the European Communities Operational quantities for use in external radiation
protection measurements. An investigation of concepts and principles. Radiological Protection-27,
Report Eur 8346 EN (European Communities:Luxembourg) (1983).

2206
2207

J. L. Conlin et al., Listing of Available ACE Data Tables,Los Alamos National Laboratory, Los Alamos,
New Mexico, LA-UR-13-21822, Issued June 5, 2005.(Rev.1)

2208
2209
2210

Daures, J. Gouriou, J. and Bordy, J-M. Monte carlo determination of the conversion coefficients
Hp(3)/Ka in a right cylinder phantom with penelope code. comparison with "mcnp"
simulations“ Radiat. Prot. Dosim. 144(1-4):37-42 (2011).

2211

Daures, J., Gouriou, J. and .Bordy, J-M. Personal Communication (2017).

2212
2213
2214

Dimbylow, P.J. and Francis, T.M. The effect of photon scatter and consequent electron build-up in air on
the calculation of dose equivalent quantities in the ICRU sphere for photon energies from 0.662 to 10
MeV, Phys. Med. Biol. 28, 817-828, (1983).

2215
2216

Dimbylow, P.J. and Francis, T.M. The calculation of dose equivalent quantities in the ICRU sphere forphoton energies from 0.01 to 10 MeV, Radiat. Prot. Dosim. 9, 49-53, (1984).

2217
2218

Endo, A. Operational quantities and new approach by ICRU. Proceedings of the Third International
Symposium on the System of Radiological Protection, Ann. ICRP 45(1S), 178-187 (2016a).

2219

Endo, A. Personal Communication (2016b).

2220
2221

Endo, A. Calculation of Fluence-to-Effective Dose Conversion Coefficients for the Operational
Quantity Proposed by ICRU RC26. Radiat. Prot. Dosim. 175, 378-387 (2017).

2222
2223

Ferrari, A. and Pelliccioni, M., On the conversion coefficients from fluence to ambient dose equivalent,
Radiat. Prot. Dosim. 51, 251-255, (1994).

2224
2225
2226

Ferrari, F and Gualdrini, G. Eye Lens Dosimetry for Electrons. Hp(3) per unit fluence conversion
coefficients for electrons from800 keV to 10 MeV based on MCNPX simulations on a cylindricalphantom ENEA - Radiation Protection Institute Report RT/2012/6/ENEA (2012).

2227
2228

Ferrari, A., Sala, P.R., Fassò, A., and Ranft, J. FLUKA: A Multi-particle Transport Code, CERN-200510, INFN/TC_05/11, SLAC-R-773 (2005).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2229
2230

Furihata, S. Statistical analysis of light fragment production from medium energy proton-induced
reactions, Nucl. Instrum. Meth. B171, 251–258 (2000).

2231
2232

Geissel, H., Scheidenberger, C., Malzacher, P., Kunzendorf, J., and Weick, H. ATIMA. Germany: GSI[cited 2013 Mar 4]. Available from: http://web-docs.gsi.de/˜weick/atima/

2233
2234

Goorley J.T. et al., Initial MCNP6 Release Overview - MCNP6 version 1.0, LA-UR-13-22934, April
2013

2235

Goorley J.T. et al., Initial MCNP6 Release Overview, Nuclear Technology 180, 298-315 (2013).

2236
2237
2238

Grosswendt, B and Chartier, J-L. Fluence-to-Absorbed-Dose Conversion Coefficients and AngularDependence Factors for 4-Element ICRU Tissue, Water and PMMA Slab Phantoms Irradiated by
Broad Electron Beams Physikalisch-Technische Bundesanstalt Report PTB-Bericht Dos—24 (1994).

2239
2240
2241

Gualdrini, G., Mariotti, F., Wach, S., Bilski, P.,Denoziere, M., Daures, J., Bordy, J.-M., Ferrari,
P.,Monteventi, F., Fantuzzi, E. andVanhavere, F. A New Cylindrical Phantom for Eye Lens Dosimetry
Development. Rad. Meas. 46, 1231-1234 (2011).

2242
2243
2244
2245
2246

Harrison, J.D., Balonov, M., Martin, C.J., Ortiz Lopez, P., Menzel, H-G., Simmonds, J.R., SmithBindman, R. and Wakeford, R. Use of Effective Dose. Proceedings of the Third International
Symposium on the System of Radiological Protection, Ann. ICRP 45(1S), 215-224 (2016).

2247
2248
2249

Hirayama, H., Namito, Y., Bielajew, A.F., Wilderman, S.J. and Nelson, W.R. TheEGS5 code system.
SLAC-R-730 and KEK Report 2005–8, SLAC NationalAccelerator Laboratory and High Energy
Accelerator Research Organization (2005).

2250
2251
2252

Hubbell, J. H. and Seltzer, S. M. Tables of x-ray mass attenuation coefficients and mass energyabsorption coefficients 1 keV to 20 MeV for elements Z = 1 to 92 and 48 additional substances of
dosimetric interest Report NISTIR 5632 (1995)

2253
2254

International Commission on Radiation Units and Measurements, ICRU Report 19, Radiation
Quantities and Units, (ICRU: Bethesda) (1971a).

2255
2256

International Commission on Radiation Units and Measurements, ICRU Report 20, Radiation
Protection Instrumentation and Its Application, (ICRU: Bethesda) (1971b).

2257
2258

International Commission on Radiation Units and Measurements, ICRU Report 33, Radiation
Quantities and Units, (ICRU: Bethesda) (1980).

2259
2260

International Commission on Radiation Units and Measurements. ICRU Report 39 Determination of
Dose Equivalents Resulting from External Radiation Sources, (ICRU: Bethesda) (1985).

2261
2262

International Commission on Radiation Units and Measurements. ICRU Report 43 Determination of
Dose Equivalents from External Radiation Sources- part 2, (ICRU: Bethesda) (1988).

Hertel, N.E. and Veinot, K.V. Personal Communication, (2017)

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2263
2264

International Commission on Radiation Units and Measurements. ICRU Report 47 Measurements ofDose Equivalents from External Photon and Electron Radiations, (ICRU: Bethesda) (1992).

2265
2266

International Commission on Radiation Units and Measurements, ICRU Report 51, Quantities andUnits in Radiation Protection Dosimetry, (ICRU: Bethesda) (1993).

2267
2268
2269

International Commission on Radiation Units and Measurements. Gamma-ray Spectrometry in theEnvironment. ICRU Report 53 (International Commission on Radiation Units and Measurements,
Bethesda, Maryland) (1994).

2270
2271
2272

International Commission on Radiation Units and Measurements, ICRU Report 57, Conversion
Coefficients for Use in Radiological Protection against External Radiation, (ICRU: Bethesda)(1998).

2273
2274
2275

International Commission on Radiation Units and Measurements, ICRU Report 66, Determination of
Operational Dose Equivalent Quantities for Neutrons, Journal of ICRU 1(3) (Oxford University
Press:Oxford) (2001).

2276
2277
2278

International Commission on Radiation Units and Measurements, ICRU Report 84, Reference Data for
the Validation of Doses from Cosmic-Radiation Exposure of Aircraft Crew, Journal of ICRU 10 (2)(Oxford University Press:Oxford) (2010).

2279
2280
2281

International Commission on Radiation Units and Measurements, ICRU Report 85a, Fundamental
Quantities and Units for Ionizing Radiation, Journal of ICRU 11 (11) (Oxford University
Press:Oxford) (2011).

2282
2283
2284

International Commission on Radiation Units and Measurements, Report 90, Key Data for IonizingRadiation Dosimetry: Measurement Standards and Applications, Journal of ICRU 14 (1) (Oxford
University Press:Oxford) (2014).

2285
2286

International Commission on Radiological Protection, ICRP Publication 15 Protection against Ionizing
Radiation from External Sources. (Pergamon Press: Oxford) (1969).

2287
2288
2289

International Commission on Radiological Protection, ICRP Publication 21 Protection against Ionizing
Radiation from External Sources: Supplement to ICRP Publication 15. (Pergamon Press: Oxford)(1971).

2290
2291

International Commission on Radiological Protection. ICRP Publication 26. Recommendations of theInternational Commission on Radiological Protection, (Pergamon Press: Oxford) (1977a).

2292
2293

International Commission on Radiological Protection, ICRP Publication 60, 1990 Recommendations of
the International Commission on Radiological Protection, (Pergamon Press: Oxford) (1991).

2294
2295
2296

International Commission on Radiological Protection, ICRP Publication 74, Conversion Coefficients for
Use in Radiological Protection against External Radiation, Ann. ICRP 26(3/4). (Elsevier Science:
Oxford) (1996).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2297
2298
2299

International Commission on Radiological Protection, ICRP Publication 89, Basic Anatomical andPhysiological Data for use in Radiological Protection, Ann. ICRP 32 (3/4). (Elsevier Science:
Oxford) (2002).

2300
2301
2302

International Commission on Radiological Protection,ICRP Publication 103, The 2007
Recommendations of the International Commission on Radiological Protection.. Ann, ICRP (Elsevier
Science: Oxford) (2007).

2303
2304

International Commission on Radiological Protection Adult Reference Computational Phantoms, ICRP
Publication 110. Ann. ICRP (Elsevier Science: Oxford) (2009).

2305
2306
2307

International Commission on Radiological Protection Conversion Coefficients for RadiologicalProtection for External Radiation Exposures, ICRP Publication 116. Ann. ICRP (Elsevier Science:
Oxford) (2010).

2308
2309
2310
2311

International Commission on Radiological Protection Statement on Tissue Reactions / Early andLate Effects of Radiation in Normal Tissues and Organs – Threshold Doses for Tissue Reactions in
a Radiation Protection Context, ICRP Publication 118. Ann. ICRP 41 (1/2) (Elsevier Science:
Oxford) (2012).

2312
2313

International Commission on Radiological Protection Assessment of Radiation Exposure of Astronautsin Space, ICRP Publication 123. Ann. ICRP 42 (4) (Elsevier Science: Oxford) (2013).

2314
2315

International Commission on Radiological Protection Radiological Protection from Cosmic Radiation in
Aviation, ICRP Publication 132. Ann. ICRP 45 (1) (Elsevier Science: Oxford) (2016).

2316
2317
2318

International Organization for Standardization, ISO 8529-3:1998, Reference neutron radiations -- Part
3: Calibration of area and personal dosemeters and the measurement of their response as a functionof energy and angle of incidence. (ISO Geneva, Switzerland) (1998).

2319
2320
2321
2322

International Organization for Standardization, ISO 4037-3:1999, X and gamma reference radiation for
calibrating dosemeters and doserate meters and for determining their response as a function ofphoton energy — Part 3: Calibration of area and personal dosemeters and the measurement of their
response as a function of energy and angle of incidence. (ISO Geneva, Switzerland) (1999).

2323
2324
2325
2326

International Organization for Standardization, ISO 6980-3:2006, Nuclear energy -- Reference betaparticle radiation -- Part 3: Calibration of area and personal dosemeters and the determination of
their response as a function of beta radiation energy and angle of incidence, (ISO Geneva,
Switzerland) (2006).

2327
2328

International Organization for Standardization, ISO 29661:2012,Reference radiation fields for radiation
protection — Definitions and fundamental concepts, (ISO Geneva, Switzerland) (2012).

2329
2330

Jahr, R. Hollnagel, R.A., and Siebert, B.R.L., A conceptual physical basis for monitoring externalradiation, Radiat. Prot. Dosim. 1, 299-304, (1981).

2331
2332
2333

Kawrakow, I., Mainegra-Hing, E., Rogers, D.W.O., Tessier, F. and Walters, B.R.B., The EGSnrc Code
System: Monte Carlo Simulation of Electron and Photon Transport. PIRS Report 701. National
Research Council of Canada, Ottawa. (2013).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2334
2335

Kawrakow, I. Electron impact ionization cross sections for EGSnrc. Med. Phys. 29, 1230 (2002).

2336
2337

Kim, J. O. and Kim, J. K. Dose equivalent per unit fluence near the surface of the ICRU phantom byincluding the secondary electron transport for photons. Radiat. Prot. Dosim. 83(3), 211–219 (1999).

2338
2339
2340
2341
2342
2343
2344
2345
2346
2347
2348
2349
2350
2351
2352
2353
2354
2355
2356
2357
2358
2359
2360
2361
2362
2363
2364
2365
2366
2367
2368
2369
2370
2371
2372
2373
2374
2375
2376
2377
2378
2379
2380

Koch, H.W., Motz, J.W., 1959. Bremsstahlung cross-section formulas and related data. Rev. Mod.
Phys.31, 920–955.
Nara, Y., Otuka, H., Ohnishi, A., Niita, K., and Chiba, S. Relativistic nuclear collisions at 10 A GeV
energies from p+Be to Au+Au with the hadronic cascade model, Phys. Rev. C61, 024901 (1999).
National Council on Radiation Protection and Measurements NCRP Report 38 Protection against
neutron radiation, (NCRP:Washington) (1971).
Nelson, W.R., Hirayama, H., Rogers, D.W.O. The EGS4 Code System. SLAC Report 265. Stanford
Linear Accelerator Center, Stanford, CA (1985).
Niita. K., Chiba, S., Maruyama, T., Maruyama, T., Takada, H., Fukahori, T., Nakahara, Y., and Iwamoto,
A. Analysis of the (N,Xn’) reactions by quantum molecular dynamics plus statistical decay model,
Phys. Rev. C52, 2620–2635 (1995).
Nuclear Regulatory Authority. Report on the Investigation for Distributions of Radioactive Substances
Released from the TEPCO Fukushima Daiichi NuclearPower Plant Accident. Available from:http://radioactivity.nsr.go.jp/ja/list/338/list-1.html. (Japanese) (2012).
Otto, T. Personal Communication (2017).
Pelliccioni, M. Fluence to dose equivalent conversion data and Radiation Weighting Factors for HighEnergy Radiation. Radiat. Prot. Dosim. 77, 159 - 170 (1998).
Pelliccioni, M. Overview of Fluence-to-Effective Dose and Fluence-to-Ambient Dose Equivalent
Conversion Coefficients for High Energy Radiation Calculated using the FLUKA Code Radiat. Prot.
Dosim. 88, 279-297 (2000).
Pelowitz D.B. (ed.), MCNP6 USER’S MANUAL Version 1.0, Manual Rev. 0, Los Alamos National
Laboratory, Los Alamos, New Mexico, LA-CP-13-00634, Rev. 0, May 2013.
Petoussi-Henss, N., Schlattl, H., Zankl, M., Endo, A. and Saito, K. Organ Doses from Environmental
Exposures Calculated using Voxel Phantoms of Adults and Children, Phys. Med. Biol. 57, 5679-5713(2012).
Saito, K., Ishigure. N., Petoussi-Henss, N. and Schlattl, H. Effective Dose Conversion Coefficients forRadionuclides Exponentially Distributed in the Ground, Radiat. Environ. Biophys. 51, 411-423(2012).
Saito, K. and Petoussi-Henss, N. Ambient Dose Equivalent Conversion Coefficients for Radionuclides
Exponentially Distributed in the Ground, J. Nucl. Sci. Technol. 51, 1274-1287 (2014).

FINAL DRAFT JULY 2017

NOT TO BE REFERENCED

2381
2382
2383
2384
2385
2386

Sato, T., Niita, K., Matsuda, N., Hashimoto, S., Iwamoto, Y., Noda, S., Ogawa, T., Iwase, H.,
Nakashima, H., Fukahori, T., Okumura, K., Kai, T., Chiba, S., Furuta, T., and Sihver, L. Particle andheavy ion transport code system PHITS, Version 2.52,J. Nucl. Sci. Technol. 50, 913-923 (2013).

2387
2388

Seltzer, S.M. Calculation of Photon Mass Energy-Transfer and Mass Energy-Absorption Coefficients.
Radiation Research 136 147-170 (1993).

2389

Seltzer, S.M. Personal Communication. (2017).

2390
2391
2392
2393
2394
2395
2396
2397
2398
2399
2400
2401
2402
2403
2404

Siebert, B.R.L. and Bartlett, D.T., Proposal of an operational quantity based directly on protection
quantities, Presented at 8th Symp. Neutron Dosimetry, Paris, November 1995 (1995).

2405

Sidwell, J.M., Burlin, T.E. and Wheatley, B.M.Calculations of the absorbed dose in a phantom fromphoton fluence and some applications to radiological protection. Br. J. Radiol. 42, 522-529 (1969).

Vanhavere, F. et al. Carinou, E., Gualdrini, G., Clairand, I., Sans Merce, M., Ginjaume, M.,
Nikodemova, D., Jankowski, J., Bordy, J.-M., Rimpler, A., Wach, S., Martin, P., Struelens, L.,
Krim, S., Koukorava, C., Ferrari, P., Mariotti, F., Fantuzzi, E., Donadille, L., Itié, C., Ruiz, N.,
Carnicer, A., Fulop, M., Domienik, J., Brodecki, M., Daures, J., Barth, I., Bilski, P. ORAMED:
Optimization of Radiation Protection of Medical Staff. EURADOS Report 2012-02. ISBN 978-3943701-01-2 (2012).
Veinot,K. and Hertel, N. E. Personal Dose Equivalent Conversion coefficients for photons to 1 GeV.
Radiat Prot Dosim. 145(1) 28-35 (2011).
Weinberg, A.V. and Wigner, E.P. The Physical Theory of Neutron Chain Reactors. University of
Chicago Press, (1958).