2006
DOI: 10.1103/physreva.74.022717
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Angular distribution of characteristic photons after radiative electron capture at strong central fields

Abstract: We investigate the difference in the angular distribution of Ly-␣ 1 and K␣ 1 photons from hydrogenlike and heliumlike ions of uranium after radiative electron capture to the L shell. The strong anisotropy in the former case is changed to a very small one in the latter case. Our calculations support the observation. The effect takes place even in the limiting case of noninteracting electrons, being caused by the Pauli principle.

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Cited by 9 publications
(7 citation statements)
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“…Two-step calculations have first been performed by Scofield [23] for the REC into bare and hydrogen-like titanium and iron ions and have been extended later successfully towards the high-Z domain [27][28][29][30][31]. However, while the capture into (initially) bare ions can be treated today quite rigorously by applying exact relativistic bound and continuum (electronic) wavefunctions, some approximate methods are required to evaluate the two-electron states.…”
Section: +mentioning
confidence: 99%
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“…Two-step calculations have first been performed by Scofield [23] for the REC into bare and hydrogen-like titanium and iron ions and have been extended later successfully towards the high-Z domain [27][28][29][30][31]. However, while the capture into (initially) bare ions can be treated today quite rigorously by applying exact relativistic bound and continuum (electronic) wavefunctions, some approximate methods are required to evaluate the two-electron states.…”
Section: +mentioning
confidence: 99%
“…However, while the capture into (initially) bare ions can be treated today quite rigorously by applying exact relativistic bound and continuum (electronic) wavefunctions, some approximate methods are required to evaluate the two-electron states. Apart from the multiconfiguration Dirac-Fock (MCDF) method, which provides a systematic approach to the electronelectron interaction effects [29,30], the REC into (initially) hydrogen-like uranium ions U 90+ can still be understood within the independent particle model [31]. This model, which takes the Pauli principle into account, should be well justified for the REC of heavy ions since the interelectronic effects are much weaker in the high-Z domain than the electron-nucleus interaction.…”
Section: +mentioning
confidence: 99%
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“…͓3,[17][18][19] In the first step, therefore, an excited level of the projectiles can be formed either by electron capture, collisional excitation or inner-shell ionization processes. Since in ion-atom collisions at storage rings the ion momentum determines the only preferred direction of the overall system, the resulting ion may appear to be aligned along this direction.…”
Section: Theoretical Backgroundmentioning
confidence: 99%
“…1 S 0 electric dipole (E1) and 3 P 2 ? 1 S 0 magnetic quadrupole (M2) transitions, both of which contribute to the Ka 1 radiation [10][11][12].…”
Section: Introductionmentioning
confidence: 99%