Import Geant4 11.0.0 source tree

This commit is contained in:
Gabriele Cosmo
2021-12-12 17:16:06 +01:00
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The photo-evaporation database contains nuclear deexcitation data starting
from a given nuclear level. Each file contains data for a given isotope,
identified by Z and A.
The database must first be downloaded from
http://geant4.web.cern.ch/geant4/support/download.shtml
and stored in a local directory. The environment variable
G4LEVELGAMMADATA must then be set to point to this directory.
**************************************************
Each line describes a de-excitation *step* from a given energy level to a lower
one (which might be the ground state). It contains data for gamma de-excitation
and internal conversion. Notice that if multiple de-excitation
channels are allowed for the starting energy level, these channels will be
described in more lines (all having the same starting level).
Each line contains 17 columns:
1) Energy of the starting nuclear level (keV)
As mentioned before, it is possible to have more lines describing the same
starting level, in the case where multiple de-excitation schemes are
allowed.
2) Energy of the transition (keV)
This is the energy difference between the initial and the final level.
3) Gamma transition probability (Ig in %)
Note1: if the probability is less than minProbability = 1e-8%, it is forced
to be 1e-8%.
Note2: see column 7 how total branching ratio is computed.
4) Polarity
Spin-parity variation in the transition
[never used in real simulation]
5) Level half-life (s)
6) Angular Momentum
Spin of the initial level
[never used in real simulation]
7) Total internal conversion coefficient : alpha = Ic/Ig
Note1: total transition is the sum of gamma de-excitation and internal
conversion. Therefore total branching ratio is proportional to
(1+alpha)*Ig
Note2: total branching ratios from a given level do not always sum up to
100%. They are re-normalized internally.
Note3: relative probabilities for gamma de-excitation and internal conversion
are 1/(1+alpha) and alpha/(1+alpha) respectively
8-17) Partial conversion probabilities for
K-shell
L1-3 shells
M1-5 shells
Outer shells (shellID = 9 is used, when applicable)
Note: if the nuclear excitation energy does not match any of the known levels,
the *nearest* level is always considered. In G4RadioactiveDecay,
metastable states are treated correctly if the excitation energy is
within 2.0 keV of the values in $G4RADIOACTIVEDATA.
For instance: take file $G4LEVELGAMMADATA/z28.a60 (Ni-60)
Co-60 radioactive decay populates the 1332.5080-keV level of
Ni-60 (0.12%) or the 2505.7480-keV level of Ni-60 (99.88%).
Deexcitation from the 2505.7480-keV level is described in lines
6-8 of $G4LEVELGAMMADATA/z28.a60 (Ni-60)
Here, internal conversion coefficients are negligeable (column 7)
Therefore the nucleus will release
1) 347 keV with 7.6e-3% probability, ending up in the 2158-keV level
(following de-excitation hence takes place, lines 2-4 of the file)
2) 1173 keV with 100% probability, ending up in the 1332-keV
excited state (following de-excitation hence takes place, line 1)
3) 2505 keV with 2e-6% probability ending up in the ground state.
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The tuning of resonances can still improve in a iteration on short-lived particles.
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This README file provides instructions for reading the radioactive decay
schemes in the files zXX.aYYY found in the directory RadioactiveDecay3.2
(most recent version). This directory, as well as previous versions, is
available from the Geant4 download page
http://geant4.web.cern.ch/geant4/support/download.shtml
under the Data files heading. In order to use the radioactive decay module
correctly, you must download and unpack the above directory in your local
area, and set the environment variable
G4RADIOACTIVEDATA
to point to it.
**************************************************************************
In each of the files, lines beginning with either a 'W' or a '#' are
comments.
Lines beginning with a 'P' are headers, each of which describes a level of
the nucleus. The first number is the excitation energy in keV, the second
is the half life in seconds. Indented lines under the 'P' lines are decay
modes for that excitation. There are two type of records here,
distinguished by the number of columns.
If there are 3 columns only, this is a header which describes all decays of
that type from this level. The first column is the decay mode, the second
column is zero, and the third column in the branching ratio to this mode,
as a fraction of unity. Therefore, the third columns of all the 3-column
records under a given 'P' line should sum to 1.0.
If there are four columns, this is a record which describes a subset of the
decay type, specific to a given lower level in the daughter species. The
first column is the decay type, the second column is the excitation level
of the daughter (in keV), and the third column is the branching ratio as a
percentage (! note... not a fraction of unity) of the total branching ratio
which came from the 3-column record for this decay.