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dc.contributor.author |
Kahoula, B. |
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dc.contributor.author |
Kasric, Y. |
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dc.contributor.author |
Sahnounea |
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dc.contributor.author |
Deghfele |
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dc.contributor.author |
Khalfallaha |
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dc.contributor.author |
Sampaiogand |
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dc.date.accessioned |
2023-01-12T16:49:48Z |
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dc.date.available |
2023-01-12T16:49:48Z |
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dc.date.issued |
2016-12-14 |
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dc.identifier.uri |
http://depot.umc.edu.dz/handle/123456789/14003 |
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dc.description.abstract |
In this work, we derive the K-shell fluorescence yield using a Dirac-Fock model. To compute, radiationless and radiative transition rates we have used the MCDF code of Desclaux and Indelicato [1-3]. The wave functions were calculated in the single-configuration approach with magnetic (Gaunt) and first-order retardation terms of the Breit interaction included in the self-consistent variational method. Higher-order Breit retardation terms were added as perturbations. Regarding the QED contributions, the one-electron self-energy is evaluated using the values of Mohr and Kim [4-5] and the self-energy screening is treated with using the Welton method reported by Indelicato [1]. Vacuum polarization is included in the calculations taking the following approach: the Uelhing contribution is evaluated to all orders by being included in the self-consistent field while higher order corrections are accounted for as perturbations. The continuum electron wave function in the final state is evaluated by solving the Dirac-Fock equations with the full exchange potential and is normalized to represent one ejected electron per unit energy. The results are compared with available data from other authors. |
fr_FR |
dc.language.iso |
en |
fr_FR |
dc.publisher |
Université Frères Mentouri - Constantine 1 |
fr_FR |
dc.subject |
K-shell fluorescence yield |
fr_FR |
dc.subject |
radiationless and radiative transtion rates |
fr_FR |
dc.subject |
Dirac-Fock calculations |
fr_FR |
dc.title |
Relativistic K shell decay rates and fluorescence yield for Fe |
fr_FR |
dc.type |
Article |
fr_FR |
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