Import Geant4 11.0.0 source tree
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The photo-evaporation database contains nuclear deexcitation data starting
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from a given nuclear level. Each file contains data for a given isotope,
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identified by Z and A.
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The database must first be downloaded from
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http://geant4.web.cern.ch/geant4/support/download.shtml
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and stored in a local directory. The environment variable
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G4LEVELGAMMADATA must then be set to point to this directory.
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**************************************************
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Each line describes a de-excitation *step* from a given energy level to a lower
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one (which might be the ground state). It contains data for gamma de-excitation
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and internal conversion. Notice that if multiple de-excitation
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channels are allowed for the starting energy level, these channels will be
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described in more lines (all having the same starting level).
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Each line contains 17 columns:
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1) Energy of the starting nuclear level (keV)
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As mentioned before, it is possible to have more lines describing the same
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starting level, in the case where multiple de-excitation schemes are
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allowed.
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2) Energy of the transition (keV)
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This is the energy difference between the initial and the final level.
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3) Gamma transition probability (Ig in %)
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Note1: if the probability is less than minProbability = 1e-8%, it is forced
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to be 1e-8%.
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Note2: see column 7 how total branching ratio is computed.
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4) Polarity
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Spin-parity variation in the transition
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[never used in real simulation]
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5) Level half-life (s)
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6) Angular Momentum
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Spin of the initial level
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[never used in real simulation]
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7) Total internal conversion coefficient : alpha = Ic/Ig
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Note1: total transition is the sum of gamma de-excitation and internal
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conversion. Therefore total branching ratio is proportional to
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(1+alpha)*Ig
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Note2: total branching ratios from a given level do not always sum up to
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100%. They are re-normalized internally.
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Note3: relative probabilities for gamma de-excitation and internal conversion
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are 1/(1+alpha) and alpha/(1+alpha) respectively
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8-17) Partial conversion probabilities for
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K-shell
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L1-3 shells
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M1-5 shells
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Outer shells (shellID = 9 is used, when applicable)
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Note: if the nuclear excitation energy does not match any of the known levels,
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the *nearest* level is always considered. In G4RadioactiveDecay,
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metastable states are treated correctly if the excitation energy is
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within 2.0 keV of the values in $G4RADIOACTIVEDATA.
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For instance: take file $G4LEVELGAMMADATA/z28.a60 (Ni-60)
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Co-60 radioactive decay populates the 1332.5080-keV level of
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Ni-60 (0.12%) or the 2505.7480-keV level of Ni-60 (99.88%).
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Deexcitation from the 2505.7480-keV level is described in lines
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6-8 of $G4LEVELGAMMADATA/z28.a60 (Ni-60)
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Here, internal conversion coefficients are negligeable (column 7)
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Therefore the nucleus will release
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1) 347 keV with 7.6e-3% probability, ending up in the 2158-keV level
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(following de-excitation hence takes place, lines 2-4 of the file)
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2) 1173 keV with 100% probability, ending up in the 1332-keV
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excited state (following de-excitation hence takes place, line 1)
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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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@@ -0,0 +1,38 @@
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This README file provides instructions for reading the radioactive decay
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schemes in the files zXX.aYYY found in the directory RadioactiveDecay3.2
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(most recent version). This directory, as well as previous versions, is
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available from the Geant4 download page
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http://geant4.web.cern.ch/geant4/support/download.shtml
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under the Data files heading. In order to use the radioactive decay module
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correctly, you must download and unpack the above directory in your local
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area, and set the environment variable
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G4RADIOACTIVEDATA
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to point to it.
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**************************************************************************
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In each of the files, lines beginning with either a 'W' or a '#' are
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comments.
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Lines beginning with a 'P' are headers, each of which describes a level of
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the nucleus. The first number is the excitation energy in keV, the second
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is the half life in seconds. Indented lines under the 'P' lines are decay
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modes for that excitation. There are two type of records here,
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distinguished by the number of columns.
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If there are 3 columns only, this is a header which describes all decays of
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that type from this level. The first column is the decay mode, the second
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column is zero, and the third column in the branching ratio to this mode,
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as a fraction of unity. Therefore, the third columns of all the 3-column
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records under a given 'P' line should sum to 1.0.
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If there are four columns, this is a record which describes a subset of the
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decay type, specific to a given lower level in the daughter species. The
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first column is the decay type, the second column is the excitation level
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of the daughter (in keV), and the third column is the branching ratio as a
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percentage (! note... not a fraction of unity) of the total branching ratio
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which came from the 3-column record for this decay.
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