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[SF7 Particle Considered] [SF8 Modifiers] [SF9 data Types] [Cinda]
(CUM) Compiler uncertain if cumulative
Application of the code 'CUM' uncertain. Explanation is
obligatory.
To be used only with process codes 'F' or 'X'
(DEF) Uncertain if reaction channel defined
Uncertain from reference whether reaction channel is
defined or whether outgoing particles represent only
sum of emitted nucleons.
=== Not to be used with process codes 'X' or 'F'.
So far used only for charged particle data
(M) Uncertain if formation via isomeric trans. included
Whether formation via isomeric transition is included
is regarded by the compiler as uncertain. Explanation
is obligatory.
1 Channel 1, e.g., in Reich-Moore res.pars.
2 Channel 2, e.g., in Reich-Moore res.pars.
20 Rank and projection (kq) f.tensor anal.p.
21 Rank and projection (kq) f.tensor anal.p.
22 Rank and projection (kq) f.tensor anal.p.
3 Channel 3, e.g., in Reich-Moore res.pars.
4 Channel 4, e.g., in Reich-Moore res.pars.
BA Bound atom
BIN Binary fission
CHG Total element yield (of fission products)
CHN Total chain
CN Compound-nucleus part
COH Coherent
CON For a range of continuum gammas, discrete gammas exclud
CUM Cumulative production of product nucleus
(Cumulative) Production of the product nucleus via
direct formation and radioactive decay.
To be used only with process codes 'F' or 'X'.
DI Direct-interaction part
DIS For a range of discrete gammas, continuum gammas exclud
DL Delayed
For use in fission.
EM Emission cross section (excluding elastic scattering)
===Use only when outgoing particle considered equals
the incident particle
EP For a given electric polarity component
FA Free atom
FIS High-energy fission cross section
GRP For a given half-life group
HEN High-energy component
INC Incoherent
IND Independent production of product nucleus
(Independent) Production of the product nucleus via
direct formation only. To be used only with process
codes 'F' or 'X' and only in cases where cumulative
production (SF5 = CUM) can occur also.
LEN Low-energy component
LL Longitudinal-longitudinal (zz) component
Beam and target spins parallel to beam direction in
scattering plane (=zz)
LON Longitudinally polarized
LP For longitudinal component of linear momentum
LS Longitudinal-sideward (zx) component
M+ Including formation via isomeric transition
M- Excluding formation via isomeric transition
MAS Total mass (for yields of fission fragments)
MP For a given magnetic polarity component
NL Normal-longitudinal (yz) component
NN Normal-normal (yy) component
Beam and target spins normal to scattering plane
(=yy)
NUM For number of outgoing particles
PAR Partial
leaving the residual nucleus in a specific level or
emitting a specific gamma or particle group.
PM+ Paramagnetic effects included
(for thermal scattering)
POT Potential
(for scattering)
PR Prompt
(for use in fission)
PRE Primary
(for fission product yields)
QTR Quaternary fission
SEC Secondary
(for fission product yields)
SEQ Particle sequence as specified in SF3
Indicates that the sequence of outgoing particles is
as specified in subfield 3.
SL Sideward-longitudinal (xz) component
Beam spin perpendicular, target spin parallel to
beam direction in scattering plane
SPL Spallation cross section
SS Sideward-sideward (xx) component
Target and beam spins perpendicular to beam
direction in scattering plane
TER Ternary fission
TP For transverse component of linear momentum
TRS Transversely polarized
UND Reaction channel undefined
outgoing particles represent only sum of emitted
nucleons.
===Not to be used with process codes 'X' or 'F'.
So far used only for charged particle data.
UNW Unweighted production cross section
not weighted by multiplicity of outgoing particle