1997
DOI: 10.1103/physreva.55.3491
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Elastic collisions and rotational excitation in positron scattering fromCO2molecules

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Cited by 19 publications
(7 citation statements)
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“…For e 1 scattering, the static interaction is repulsive and the correlation-polarization interaction is attractive, but no exchange interaction exists. Hence, the repulsive static and attractive polarization cancel out, resulting in the smaller interaction on scattering at low-to-intermediate scattering energies, as we have witnessed in the total cross section [3]. It is important, and also our present aim, to examine how these interaction potentials contribute to specific modes in vibrational excitation processes.…”
mentioning
confidence: 83%
“…For e 1 scattering, the static interaction is repulsive and the correlation-polarization interaction is attractive, but no exchange interaction exists. Hence, the repulsive static and attractive polarization cancel out, resulting in the smaller interaction on scattering at low-to-intermediate scattering energies, as we have witnessed in the total cross section [3]. It is important, and also our present aim, to examine how these interaction potentials contribute to specific modes in vibrational excitation processes.…”
mentioning
confidence: 83%
“…Numerous approaches were proposed in the past, based on modifications of the polarization potential [45], deriving the short-range interaction from electronic densities etc. [46], or expanding the scattering amplitude at low energies [43]. In the present approach we express V S (r) in terms of some boundary conditions imposed on the wave function at r → 0, while the effects resulting from the finite range of V s (r) are included explicitly in the framework of the modified effective-range theory.…”
Section: Scattering Of a Charged Particle On A Molecule And The Quant...mentioning
confidence: 99%
“…Numerous approaches were proposed in the past, based on modifications of the polarization potential [3], deriving the short-range interaction from electronic densities etc. [34], or expanding the scattering amplitude at low energies [33]. In the present approach we express V S (r) in terms of some boundary conditions imposed on the wave function at r → 0, while the effects resulting from the finite range of V S (r) are included explicitly in the framework of the modified effective-range theory.…”
Section: Introductionmentioning
confidence: 99%
“…Combining ( 9), ( 10), (34), (35) one can easily obtain the low-energy expansion of the phase shifts [11]…”
Section: Introductionmentioning
confidence: 99%