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  • The method for the evaluation of the self-energy of bound electron is proposed. The integration over four-momenta of virtual photons is done in a way that preserves manifest Lorentz invariance. The resulting expression can then be decomposed into high-and low-energy parts in a Lorentz invariant fashion. The high-energy part depends only on the behavior of the wave function of the reference state in the immediate vicinity of the nucleus and can be calculated analytically. The low-energy part depends on further details of the atomic structure and has to be calculated numerically. The results accurate at least up to alpha(Z alpha)(6) are obtained for non-S states and normalized difference n(3)Delta E-n - Delta E-1 of the S states. The method is applied to the states with the principal quantum number n ranging from 2 to 10, with the orbital quantum number l ranging from 0 to 3 and with the nuclear charges Z ranging from 1 to 30. In the cases that were already considered in literature a very good agreement with previous calculations is found, especially for the atoms with lower nuclear charges. The advantages of the present method over the previous ones are pointed out.
  • The method for the evaluation of the self-energy of bound electron is proposed. The integration over four-momenta of virtual photons is done in a way that preserves manifest Lorentz invariance. The resulting expression can then be decomposed into high-and low-energy parts in a Lorentz invariant fashion. The high-energy part depends only on the behavior of the wave function of the reference state in the immediate vicinity of the nucleus and can be calculated analytically. The low-energy part depends on further details of the atomic structure and has to be calculated numerically. The results accurate at least up to alpha(Z alpha)(6) are obtained for non-S states and normalized difference n(3)Delta E-n - Delta E-1 of the S states. The method is applied to the states with the principal quantum number n ranging from 2 to 10, with the orbital quantum number l ranging from 0 to 3 and with the nuclear charges Z ranging from 1 to 30. In the cases that were already considered in literature a very good agreement with previous calculations is found, especially for the atoms with lower nuclear charges. The advantages of the present method over the previous ones are pointed out. (en)
Title
  • Self-energy of a bound electron for excited states
  • Self-energy of a bound electron for excited states (en)
skos:prefLabel
  • Self-energy of a bound electron for excited states
  • Self-energy of a bound electron for excited states (en)
skos:notation
  • RIV/00216208:11320/12:10128523!RIV13-GA0-11320___
http://linked.open...avai/predkladatel
http://linked.open...avai/riv/aktivita
http://linked.open...avai/riv/aktivity
  • P(GAP205/10/0228), S
http://linked.open...iv/cisloPeriodika
  • 4
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  • 167348
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  • RIV/00216208:11320/12:10128523
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  • constants; atoms; hydrogenlike systems; lamb shift; radiative level shifts; order binding corrections; free propagator expansion; strong coulomb field (en)
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  • US - Spojené státy americké
http://linked.open...ontrolniKodProRIV
  • [C624D006584F]
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  • Physical Review A - Atomic Molecular and Optical Physics
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http://linked.open...UplatneniVysledku
http://linked.open...v/svazekPeriodika
  • 86
http://linked.open...iv/tvurceVysledku
  • Zamastil, Jaroslav
  • Patkóš, Vojtěch
http://linked.open...ain/vavai/riv/wos
  • 000310259600003
issn
  • 1050-2947
number of pages
http://bibframe.org/vocab/doi
  • 10.1103/PhysRevA.86.042514
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  • 11320
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