... | ... | @@ -9,12 +9,13 @@ Sternheimer's approximation (R.M. Sternheimer, Phys. Rev. 88, 851 (1952)) for th |
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Data tables are taken from [1-s2.0-0092640X84900020-main.pdf](uploads/82e2bf820f20ebfa982035c3eda960f8/1-s2.0-0092640X84900020-main.pdf), see update here [1-s2.0-S0092640X01908617-main.pdf](uploads/647767824d8c3a2d539b73591d1c6748/1-s2.0-S0092640X01908617-main.pdf)
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and electronic tables from at http://pdg.lbl.gov/2018/AtomicNuclearProperties/index.html (see EXPERTS section), the data is also copied to EnergyLoss/Properties8.dat etc.
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Shell correction are discussed here:
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Barkas paper for original shell correction: https://www.nap.edu/read/20066/chapter/8 outdated, but simple to implement.
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Shell correction are discussed by Bichsel 1992 in a more modern approach:
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[PhysRevA.46.5761.pdf](uploads/dcdaf0c5f26e0a6df81770028faa36af/PhysRevA.46.5761.pdf)
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Barkas paper for original shell correction: https://www.nap.edu/read/20066/chapter/8 outdated, but simple to implement.
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Barkas correction also describes differences between positive and negative projectiles.
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Barkas correction to the Bethe formula also describes differences between positive and negative projectiles.
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Heavy particles Z>56 require extra work, e.g. ???
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