1967
DOI: 10.1103/physrev.160.472
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Partial-Wave Scattering by Non-Spherically-Symmetric Potentials. I. General Theory of Elastic Scattering

Abstract: A general method is developed to obtain the elastic-scattering cross section of an asymmetric potential V(r) = J2iVi( r )Pi(Pz*r) where we have expanded the potential as a sum of multipoles and tii is a unit vector along the 2/-pole axis. We assume that vi(r) is effectively zero beyond a cutoff radius R and we solve the resulting set of coupled differential equations in terms of a scattering matrix S. A general expression for the scattering amplitude /(k,k') is derived in terms of the elements of S and 3j symb… Show more

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Cited by 27 publications
(8 citation statements)
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“…In that case the probabilistic interpretation of quantum mechanics, with squares of force matrix-elements, becomes transparent. Beyond that impurity limit and in a mean-field picture, which rests on projectile screening and scattering of independent electrons, a nonspherical multipole expansion [31] could be the consistent one. However, in such a treatment with nonspherical scattering potentials to determine the corresponding force-matrix elements [16], one arrives at coupled equations.…”
Section: Theory and Resultsmentioning
confidence: 99%
“…In that case the probabilistic interpretation of quantum mechanics, with squares of force matrix-elements, becomes transparent. Beyond that impurity limit and in a mean-field picture, which rests on projectile screening and scattering of independent electrons, a nonspherical multipole expansion [31] could be the consistent one. However, in such a treatment with nonspherical scattering potentials to determine the corresponding force-matrix elements [16], one arrives at coupled equations.…”
Section: Theory and Resultsmentioning
confidence: 99%
“…In the case of the (H 2 O) 4 cluster model with R′ = 7.96 Å and l = 1, r max occurs near 3.5 Å, which is far too small to be consistent with a nonvalence shape resonance. We now consider the impact of including the nonspherical electrostatic contribution to the interaction potential using the protocol of Bordman et al 48 in which the interaction potential is decomposed into contributions from different spherical harmonics. Assuming that the resonance is purely p-wave in nature, only V 0 and V 2 components can contribute to the effective radial potential.…”
Section: Resultsmentioning
confidence: 99%
“…The scattering considered in this paper is the scattering on spherically symmetric target. For non-spherically symmetric targets, the target function can be expanded by the spherical harmonic function [22]. Then the result of a non-spherically symmetric scattering is a series sum of spherically symmetric scatterings.…”
Section: Discussionmentioning
confidence: 99%