dc.contributor.author |
Kahoul, A |
|
dc.contributor.author |
Kasri, Y |
|
dc.contributor.author |
Sahnoune, Y |
|
dc.contributor.author |
Deghfel, B |
|
dc.contributor.author |
Khalfallah, F |
|
dc.contributor.author |
Sampaio, J. M |
|
dc.contributor.author |
Marques, J. P |
|
dc.date.accessioned |
2022-05-30T10:40:12Z |
|
dc.date.available |
2022-05-30T10:40:12Z |
|
dc.date.issued |
2016-12-15 |
|
dc.identifier.uri |
http://depot.umc.edu.dz/handle/123456789/12805 |
|
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 |
|
dc.language.iso |
en |
|
dc.publisher |
Université Frères Mentouri - Constantine 1 |
|
dc.subject |
K-shell fluorescence yield |
|
dc.subject |
radiationless and radiative transtion rates |
|
dc.subject |
Dirac-Fock calculations |
|
dc.title |
Relativistic K shell decay rates and fluorescence yield for Fe |
|
dc.type |
Article |
|