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Negative muon capture in very light atoms
The transition rates for unbound muons to be captured into atomic bound states are calculated as functions of (1) incident muon center-of-mass energy, (2) muon principal quantum number n, and (3) muon (final) angular momentum l, for the hydrogen, helium, and lithium atoms. These rates reflect differ...
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Published in: | Annals of physics 1974-01, Vol.86 (1), p.178-192 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The transition rates for unbound muons to be captured into atomic bound states are calculated as functions of (1) incident muon center-of-mass energy, (2) muon principal quantum number
n, and (3) muon (final) angular momentum
l, for the hydrogen, helium, and lithium atoms. These rates reflect differences in electron binding energies. At muon energies of several hundred electron volts, lithium
K-shell electrons are more likely to be ejected than the
L-shell electron, while this behavior is reversed for energies ≲ 10 eV. However, in each case when the capture rate is folded with a muon stopping power function, the result is that more than half of the unbound muons are absorbed above 75 eV. Implications for experiments which look at muon transfer processes are noted. |
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ISSN: | 0003-4916 1096-035X |
DOI: | 10.1016/0003-4916(74)90435-7 |