source: trunk/source/processes/hadronic/models/de_excitation/photon_evaporation/README-LevelGammaData @ 1350

Last change on this file since 1350 was 1350, checked in by garnier, 14 years ago

update to last version 4.9.4

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1
2The photo-evaporation database contains nuclear deexcitation data starting
3from a given nuclear level. Each file contains data for a given isotope,
4identified by Z and A.
5
6The database must first be downloaded from
7
8http://geant4.web.cern.ch/geant4/support/download.shtml
9
10and stored in a local directory.  The environment variable
11G4LEVELGAMMADATA must then be set to point to this directory.
12 
13**************************************************
14
15Each line contains a de-excitation *step* from a given energy level to a lower
16one (which might be the ground state). Notice that if multiple de-excitation
17channels are allowed for the starting energy level, these channels will be
18described in more lines (all having the same starting level).
19
20
21Each line contains 17 columns:
22
231) Energy of the starting nuclear level (keV)
24   As mentioned before, it is possible to have more lines describing the same
25   starting level, in the case where multiple de-excitation schemes are
26   allowed.
27       
282) Energy of the transition (keV)
29   This is the energy difference between the initial and the final level.
30
313) Transition probability (%)
32   Note1: if the probability is less than  minProbability = 1e-8%, it is forced
33          to be 1e-8%.
34   Note2: transition probabilities from a given level do not always sum up to
35          100% exactly. They are re-normalized internally.
36
374) Polarity
38   Spin-parity variation in the transition
39   [never used in real simulation]
40
415) Level half-life (s)
42
436) Angular Momentum
44   Spin of the initial level
45   [never used in real simulation]
46
477) Total internal conversion probability
48   Note: the value in item (3) is the *transition* probability, so the
49         actual *gamma* probability is calculated taking into account the
50         probability of internal conversion.
51
528-17) Partial conversion probabilities for
53        K-shell
54        L1-3 shells
55        M1-5 shells
56        Outer shells (shellID = 9 is used, when applicable)
57
58Note: if the nuclear excitation energy does not match any of the known levels,
59      the *nearest* level is always considered.  In G4RadioactiveDecay,
60      metastable states are treated correctly if the excitation energy is
61      within 2.0 keV of the values in $G4RADIOACTIVEDATA.
62
63      For instance: take file $G4LEVELGAMMADATA/z28.a60 (Ni-60)
64      Co-60 radioactive decay populates the 1332.5080-keV level of
65      Ni-60 (0.12%) or the 2505.7480-keV level of Ni-60 (99.88%).
66
67      Deexcitation from the 2505.7480-keV level is described in lines
68      6-8 of $G4LEVELGAMMADATA/z28.a60 (Ni-60)
69      The nucleus will release
70      1) 347 keV with 7.6e-3% probability, ending up in the 2158-keV level
71      (following de-excitation hence takes place, lines 2-4 of the file)
72      2) 1173 keV with 100% probability, ending up in the 1332-keV
73      excited state (following de-excitation hence takes place, line 1)
74      2) 2505 keV with 2e-6% probability ending up in the ground state.
75
76
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