1975
DOI: 10.1063/1.431598
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Approximations for the exchange potential in electron scattering

Abstract: Four new exchange potentials (the semiclassical exchange approximation, the asymptotically adjusted free-electron–gas exchange approximation, the second-order free-electron–gas exchange approximation, and the high-energy exchange approximation) are derived. Calculations are performed for elastic electron scattering from helium and argon. The results are compared to one another and to calculations using Hara’s free-electron–gas approximation and the exact nonlocal exchange potential. Three of the approximations… Show more

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Cited by 460 publications
(143 citation statements)
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“…To construct this complex potential for each atom, the real part of the potential is represented by the sum of three terms: (i) a static term derived from a Hartree-Fock calculation of the atomic charge distribution, 27 (ii) an exchange term to account for the indistinguishability of the incident and target electrons, 28 and (iii) a polarisation term 29 for the long-range interactions which depend on the target dipole polarisability. 26 The imaginary part, following the procedure of Staszewska et al, 30 then treats inelastic scattering as electron-electron collisions.…”
Section: Numerical Considerationsmentioning
confidence: 99%
“…To construct this complex potential for each atom, the real part of the potential is represented by the sum of three terms: (i) a static term derived from a Hartree-Fock calculation of the atomic charge distribution, 27 (ii) an exchange term to account for the indistinguishability of the incident and target electrons, 28 and (iii) a polarisation term 29 for the long-range interactions which depend on the target dipole polarisability. 26 The imaginary part, following the procedure of Staszewska et al, 30 then treats inelastic scattering as electron-electron collisions.…”
Section: Numerical Considerationsmentioning
confidence: 99%
“…To construct this complex potential for each atom, we followed the procedure proposed by Staszewska et al, 63 where the real part of the potential is represented by the sum of three terms: (i) a static term derived from a Hartree-Fock calculation of the atomic charge density distribution, 64 (ii) an exchange term to account for the indistinguishability of the incident and target electrons, 65 and (iii) a polarization term 66 for the long-range interactions which depends on the target polarizability α. 18 The imaginary part then treats inelastic scattering as electron-electron collisions.…”
Section: Theoretical Outline and Numerical Analysismentioning
confidence: 99%
“…͓4͔, and references therein͒. In the present calculations, we use the exchange potential of Furness and McCarthy ͓6,7,25͔, which is derived directly from the formal expression of the nonlocal exchange interaction by using a WKB-like approximation for the wave functions:…”
Section: Optical Potentialmentioning
confidence: 99%