1974
DOI: 10.1021/ja00822a001
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Theoretical study of inner-shell photoionization cross sections and angular distributions

Abstract: Atomic photoionization cross sections and asymmetry parameters are calculated using a simple oneelectron model potential consisting of the positive nuclear charge at the origin surrounded by a series of negatively charged spherical shells. The radial Schrodinger equation is solved exactly for unbound states of the potential using Whittaker functions. Parameters for the model potential (shell radii and charges) are fitted using SCF charge densities. Applications are made to inner-shell ionizations of atoms and … Show more

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Cited by 28 publications
(9 citation statements)
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“…Because the results for the monoxide and sesquioxide are the same within experimental error, it can be assumed that their electron-loss processes are very similar. Chapman and Lohr (30) have predicted that the cross section should increase with increasing binding energy (higher oxidation states). The observed variation, however, is too small to assign to differences in the oxidation state of the ion.…”
Section: Resultsmentioning
confidence: 99%
“…Because the results for the monoxide and sesquioxide are the same within experimental error, it can be assumed that their electron-loss processes are very similar. Chapman and Lohr (30) have predicted that the cross section should increase with increasing binding energy (higher oxidation states). The observed variation, however, is too small to assign to differences in the oxidation state of the ion.…”
Section: Resultsmentioning
confidence: 99%
“…(1). The angular distribution of the emitted photoelectron is calculated by the following equation [16]:…”
Section: Simulation Modelmentioning
confidence: 99%
“…This field has been used by McGuire [19] and by Chapman and Lohr [20] in calculating continuum wave-functions and photoionization cross sections. Since the field is Coulombic in each region of space, hydrogenic wave-functions matched at each shell radius form exact solutions of the Schrodinger equation.…”
Section: X[(ha-p)(n+n')-h(n'-l)(a+p)] (2 1)mentioning
confidence: 99%
“…The term in T involving,radial * While [A,, TI contains fourth derivatives with respect to Cartesian coordinates, it is easily shown to contain no derivatives higher than the third with respect to the radial coordinate r. As described in [20], not only are the piecewise Coulombic wave-functions and their first derivatives with respect to r continuous at the shell radii, but also their second derivatives are continuous. The jump discontinuities in the third radial derivatives at the shell radii are finite, so that a Dirac 6 function does not appear until fourth radial derivatives are taken.…”
Section: P = (E2p/h)[z":e(a -R ) +~$~~( R -A ) ] (30)mentioning
confidence: 99%