Energy-momentum structure of the krypton valence shell by electron-momentum spectroscopy

Momentum distributions and spectroscopic factors are obtained in a high-resolution electron-momentum spectroscopy study of krypton at 1000 eV. The shapes and relative magnitudes of the momentum profiles are in good agreement with the results of calculations made within the distorted-wave impulse app...

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Veröffentlicht in:Physical Review A 1996-06, Vol.53 (6), p.4205-4214
Hauptverfasser: Nicholson, R, Braidwood, SW, McCarthy, IE, Weigold, E, Brunger, MJ
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container_end_page 4214
container_issue 6
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container_title Physical Review A
container_volume 53
creator Nicholson, R
Braidwood, SW
McCarthy, IE
Weigold, E
Brunger, MJ
description Momentum distributions and spectroscopic factors are obtained in a high-resolution electron-momentum spectroscopy study of krypton at 1000 eV. The shapes and relative magnitudes of the momentum profiles are in good agreement with the results of calculations made within the distorted-wave impulse approximation (DWIA) framework. The DWIA describes the relative magnitudes of the 4{ital p} and 4{ital s} manifolds as well as giving a good representation of the shapes of the respective 4{ital p} and 4{ital s} cross sections. Results for the momentum profiles belonging to excited {sup 2}{ital P}{sup {ital o}} and {sup 2}{ital S}{sup {ital e}} manifolds are also presented. Spectroscopic factors for transitions belonging to the {sup 2}{ital P}{sup {ital o}} and {sup 2}{ital S}{sup {ital e}} manifolds are assigned up to a binding energy of 42 eV. The spectroscopic factor for the lowest 4{ital s} transition is 0.51{plus_minus}0.01, whereas that for the ground-state 4{ital p} transition is 0.98{plus_minus}0.01. Comparisons of the present binding energies and spectroscopic factors are made against the results of several many-body calculations and photoelectron spectroscopy results. In addition, we outline a procedure, utilizing the experimental 4{ital p} and 4{ital s} manifold cross sections, that provides information on possible initial-state configuration-interaction effects in krypton. {copyright} {ital 1996 The American Physical Society.}
doi_str_mv 10.1103/physreva.53.4205
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The shapes and relative magnitudes of the momentum profiles are in good agreement with the results of calculations made within the distorted-wave impulse approximation (DWIA) framework. The DWIA describes the relative magnitudes of the 4{ital p} and 4{ital s} manifolds as well as giving a good representation of the shapes of the respective 4{ital p} and 4{ital s} cross sections. Results for the momentum profiles belonging to excited {sup 2}{ital P}{sup {ital o}} and {sup 2}{ital S}{sup {ital e}} manifolds are also presented. Spectroscopic factors for transitions belonging to the {sup 2}{ital P}{sup {ital o}} and {sup 2}{ital S}{sup {ital e}} manifolds are assigned up to a binding energy of 42 eV. The spectroscopic factor for the lowest 4{ital s} transition is 0.51{plus_minus}0.01, whereas that for the ground-state 4{ital p} transition is 0.98{plus_minus}0.01. 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The shapes and relative magnitudes of the momentum profiles are in good agreement with the results of calculations made within the distorted-wave impulse approximation (DWIA) framework. The DWIA describes the relative magnitudes of the 4{ital p} and 4{ital s} manifolds as well as giving a good representation of the shapes of the respective 4{ital p} and 4{ital s} cross sections. Results for the momentum profiles belonging to excited {sup 2}{ital P}{sup {ital o}} and {sup 2}{ital S}{sup {ital e}} manifolds are also presented. Spectroscopic factors for transitions belonging to the {sup 2}{ital P}{sup {ital o}} and {sup 2}{ital S}{sup {ital e}} manifolds are assigned up to a binding energy of 42 eV. The spectroscopic factor for the lowest 4{ital s} transition is 0.51{plus_minus}0.01, whereas that for the ground-state 4{ital p} transition is 0.98{plus_minus}0.01. Comparisons of the present binding energies and spectroscopic factors are made against the results of several many-body calculations and photoelectron spectroscopy results. In addition, we outline a procedure, utilizing the experimental 4{ital p} and 4{ital s} manifold cross sections, that provides information on possible initial-state configuration-interaction effects in krypton. {copyright} {ital 1996 The American Physical Society.}</abstract><cop>United States</cop><pmid>9913389</pmid><doi>10.1103/physreva.53.4205</doi><tpages>10</tpages></addata></record>
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source American Physical Society Journals
subjects ELECTRON SPECTRA
ELECTRON SPECTROSCOPY
ELECTRON-ATOM COLLISIONS
GROUND STATES
IONIZATION POTENTIAL
KRYPTON
PHOTOELECTRON SPECTROSCOPY
PHYSICS
title Energy-momentum structure of the krypton valence shell by electron-momentum spectroscopy
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