Japan Charged-Particle Nuclear Reaction Data Group
Division of Physics, Graduate School of Science
Hokkaido University
060-0810 Sapporo, JAPANE-mail: services@jcprg.org
Internet: http://www.jcprg.org/Telephone +81(JPN)-11-706-2684
Facsimile +81(JPN)-11-706-4850

Memo CP-E/074
Date:
To:
From:
Subject:

September 14, 2005
Distribution
OTSUKA Naohiko
Multiple reaction formalism

We are restricting quantities which may be coded using multiple reaction formalism to thefollowing 5 cases (see LEXFOR “Multiple reaction formalism”):
1. Resonance parameters of the same isotope and target, determined in the same analysis
2. Multiple representations of the same data:
3. Partial cross sections of a sum reactiona) Isomer data (branches, ratios, etc.) of the same reactions.
b) Compound nucleus and direct interaction parts for the same reactions.
c) High-energy fission and spallation parts for the same reactions.
d) Binary and ternary parts for fission measured.
e) Light and heavy fragment parts for a given fission yield.
4. Data measured simultaneously for the production of specific particles or nuclides
5. Data for the same reaction obtained by different types of analysis
with 3 basic constraints (See System Manual “Reaction specification”):
1. The incident projectile and the target nucleus are constant.
2. Quantities are functions of the same independent variables.
3. Quantities are integrally related to each other.
I propose addition of a new case “Components of a vector or tensor quantity” into above list.
There might be other additional categories of data to which multiple reaction formalism could
be allowed. Centres may propose such categories in the NRDC meeting in October.

Distribution:
S. Babykina, CAJaD
F.E. Chukreev, CAJaD
A. Hasegawa, JAERIS. Maev, CJD
C. Nordborg, NEA-DB
O. Schwerer, NDS
V. Varlamov, CDFE
V. Zerkin, NDS

A. Blokhin, CJD
S. Dunaeva, NDS
H. Henriksson, NEA-DB
V.N. Manokhin, CJD
P. Obložinský, NNDC
S. Tákacs, ATOMKI
M. Vlasov, KINR
Y.X. Zhuang, CNDC

J.H. Chang, KAERI
Z.G. Ge, CNDC
A. Kaltchenko, KINR
V. McLane, NNDC
A. Ohnishi, JCPRG
S. Taova, VNIIEF
M. Wirtz, NDS
EXFOR, NEA-DB

M. Chiba, JCPRG
O. Gritzay, KINR
K. Katō, JCPRG
M. Mikhaylyukova, CJD
D. Rochman, NNDC
T. Tárkányi, ATOMKI
H.W. Yu, CNDC
JCPRG Distribution

Sample of coded entry (E1898.008)
T. Wakasa et al., Phys. Rev. C69 (2004) 044602 Fig.2
SUBENT
BIB
REACTION

E1898008
20050813
E189800800001
511E189800800002
1(1-H-2(P,X)0-NN-1,SS,POL/DA/DE,,D)
E189800800003
2(1-H-2(P,X)0-NN-1,SL,POL/DA/DE,,D)
E189800800004
3(1-H-2(P,X)0-NN-1,NN,POL/DA/DE,,D)
E189800800005
EN-SECANG is polar angle between beam and neutron inE189800800006
laboratory system
E189800800007(E-DGD,N) Energy transfer from projectile to target
E189800800008
SAMPLE
Target-thickness: 662 mg/cm2 for CD2 and 682 mg/cm2
E189800800009
for C
E189800800010
ERR-ANALYS (ERR-S) Statistical uncertainty
E189800800011
STATUS(TABLE) Data (Fig.2, p044602-4 in reference) received E189800800012
by e-mail from T.Wakasa (2004.05.24)
E189800800013
ENDBIB
110
E189800800014
COMMON33
E189800800015
EN
E-RSL
ANG
E189800800016
MEV
MEV
ADEG
E189800800017
345.0
3.0
16.0
E189800800018
ENDCOMMON30E189800800019
DATA
717
E189800800020
E-DGD
DATA
1ERR-S
1DATA
2ERR-S
2DATA
3E189800800021
ERR-S
3
E189800800022
MEV
NO-DIM
NO-DIM
NO-DIM
NO-DIM
NO-DIM
E189800800023
NO-DIM
E189800800024
20.00-0.56780.01980.02070.0216
0.0581
E189800800025
0.0221
E189800800026
25.00-0.63480.0166
0.03790.01810.1009E189800800027
0.0186
E189800800028…
167.50-0.2183
0.13840.16770.1479-0.2814
E189800800055
0.1222
E189800800056
187.50-0.04780.1709-0.0505
0.1829-0.0302
E189800800057
0.1423
E189800800058
ENDDATA380
E189800800059
ENDSUBENT
580
E189800899999