NATIONAL NUCLEAR DATA CENTER
Bldg. 197DBrookhaven National Laboratory
P. O. Box 5000
Upton, NY 11973-5000 U.S.A.
(Internet) "NNDC@BNL.GOV

Telephone: (516)344-2902
FAX: (516)344-2806

Memo CP-C/347
DATE:
TO:
FROM:
SUBJECT:

August 6, 2004
Distribution
V. McLane
Cross sections measured on thick targets.
Updated LEXFOR entry on thick target yields

As Naohiko Otsuka pointed out, the data given as cross sections measured on thick targets,and similarly, product yields, multiplicities, etc., are simply cross sections averaged over anincident energy range. Therefore, I propose we make TT a general quantity modifier andeliminate it from codes in Dictionary 36.
Update to Dictionary 34 (Modifiers)TT
GENQA Average for incident energy degraded through thick target.
An updated LEXFOR entry for Thick and Thin target yields follows. I hope have taken into
account all memos. I used the table from CP-E/044 and made some changes to make units
types more consistent. Unit types are given for data types not yet encountered to facilitate
further additions.

Distribution:
M. Chiba, Sapporo
F. E. Chukreev, CAJaD
S. Dunaeva, NDS
S. Taova, Sarov
O. Gritzay, KINR
K. Kato, JCPDG
M. Kellett, NEADB
V. N. Manokhin, CJD

S. Maev, CJD
O. Schwerer, NDS
S. Takács, ATOMKI
F. T. Tárkányi, ATOMKI
V. Varlamov, CDFE
CNDC
NNDC Distribution

Thick-Target yields

Thick- and Thin-Target Yields
Thick-target yields: yield of an outgoing particle (or radiation) measured on a target whose
thickness is such that the incident beam is either:1) completely stopped within the target,2) significantly degraded in energy,3) degraded in energy to below the threshold for producing the measured product.
Thin-target yields: yield of an outgoing particle (or radiation) measured on a target whose
thickness is such that the incident beam is less significantly degraded in energy, and which isgiven as a function of incident beam current. The incident energy range must be given in thedata table under the field headings EN-MIN and EN-MAX, or, if the final energy is not
specified, the incident energy and target thickness must be given under EN and THICKNESS.
The data are sensitive to target thickness and beam profile. The energy loss is a function ofthe stopping power (S) of the target material.
The thick target yield is given by−1

 dE ′ ( E )  dE ′Ythick ≈ ∫ σ ( E ′) E2
 dX
S = dE / dX
E0

where

E0 is the incident particle energy,
E2 is the final energy of the incident particle; either 0 if the beam is stopped in
the target, or equal to the energy of the particle exiting the target,
E΄ is the energy at a given depth in the target,
X is the target thickness in g cm-2.

Types of data compiled:
1) Saturated thick/thin-target yield: target yield measured after a long irradiation time (i.e.,longer than 3 half-lives of the product activity) and usually given as decay rate per unit ofincident beam current.
REACTION Coding: TTY in SF6
Units: a code from Dictionary 25 with dimension TTY (decay rate per unit of beam
current), e.g., MCI/MUA.
2) Production1 thick/thin-target yield: (unsaturated) target yield measured after an irradiation
time that is short compared to the product half-life and given as decay rate per unit ofincident beam current ∗ time.
REACTION Coding: TTY,,DTUnits: a code from Dictionary 25 with dimension TTT (decay rate per unit of beamcurrent ∗ time), e.g., MCI/MUAHR or DPS/MUAHR.

1Do not confuse with product yields.

Thick-Target yields
3) Physical thick/thin-target yield: target yield measured after an irradiation time that is shortcompared to the product half-life, is given as decay rate per unit of incident beam current∗ time, and has been corrected for decays during irradiation.
REACTION Coding: TTY,,PHY
Units: a code from Dictionary 25 with dimension TTT (decay rate per unit of beam
current ∗ time), e.g., MCI/MUAHR or DPS/MUAHR.
4) Other representations of thick target yieldsa) Thick Target Cross Sections: cross section measured on a thick target and notcorrected for target thickness.
REACTION Coding: SIG in SF 6; modifier TT in SF8.
Units: a code from Dictionary 25 with dimension B, e.g., MBb) Thick Target Product Yields: thick target yield of a reaction product, where:•the value is given in units of number of nuclei per incident projectile.
REACTION Coding: PY in SF 6; modifier TT in SF8.
Units: a code from Dictionary 25 with dimension YLD, e.g., PRD/INC•

the value is given in units of number of nuclei as a function of incident beamcurrent.
REACTION Coding: TTY/PY in SF 6.
Units: a code from Dictionary 25 with dimension PYT, e.g., PRD/MUAHRc) Thick Target Yield Multiplicities: yield of an outgoing particle (or radiation), where:•

the value is given as the number of particles per incident projectile.
REACTION Coding: MLT in SF 6, TT in SF8.
Units: a code from Dictionary 25 with dimension YLD, e.g., PRT/INC•the value is given as the number of particles as a function of incident beam current.
REACTION Coding: TTY/MLT in SF 6.
Units: a code from Dictionary 25 with dimension PYT, e.g., PRT/MUAHRd) Thick Target Gamma-Ray Yields: gamma spectrum, where the value is given as thenumber of particles per incident projectile as a function of gamma energy.
REACTION Coding: SPC in SF 6, TT in SF8.
Units: a code from Dictionary 25 with dimension YLD, e.g., PRT/INC
Similarly, all quantities may be given as angular distributions, excitation functions, etc. See
Table following and Dictionary 36 for a complete list of quantities.

Thick-Target yields
Unit definitions
Saturated thick target yields are most often measured as observed decay rate per unit of beam
current. Unsaturated thick target yields are most often measured as observed decay rate perunit of beam current per unit time.
Measures of beam current
Ampere:SI fundamental unit of current.
Coulomb: SI fundamental unit of charge; 1 C = 1 Ampere of current for 1 second.
Measures of decay rate
Becquerels SI fundamental unit of radioactivity; 1 Bq = 1 decay/second.
unit of radioactivity; 1 Ci = 3.7x1010 decays/second.
Curies2:
1 Bq = 2.7x10-11 Ci

Table of data types verses unit types
Type of data compiled

Saturated thick/thin-target yield
Production thick/thin-target yield andPhysical thick/thin-target yield
Cross section
Thick target cross section
Fn. of beam current
Thick target product yield Fn. of beam current
and multiplicity# of nuclei/inc.

2

The Curie has been replaced in usage by the Becquerel.

Unit type fortype
TTY

d/dA
TDA

d/dE
TDE

d2/dA/dE
TD2

TTT

TTDA

TTDE

TTD2B
BTT
PYT

DA
DATT
PYTA

DE
DETT
PYTE

DAE
DAET
PYT2

YLD

1/A

1/E

1/AE