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(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