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Dynamics of electron capture in positron‐hydrogen scattering under dense semi‐classical plasmas

The scattering dynamics of electron capture in e+$$ {\mathrm{e}}^{+} $$‐H(1 s) scattering under dense semi‐classical plasma (DSCP) environments has been investigated theoretically. Coupled multi‐channel two‐body Lippmann‐Schwinger equations have been solved by retaining e+$$ {\mathrm{e}}^{+} $$+H(1 ...

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Published in:Contributions to plasma physics (1988) 2024-11, Vol.64 (10), p.n/a
Main Authors: Das, Kamalika, Das, Netai, Ghoshal, Arijit
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description The scattering dynamics of electron capture in e+$$ {\mathrm{e}}^{+} $$‐H(1 s) scattering under dense semi‐classical plasma (DSCP) environments has been investigated theoretically. Coupled multi‐channel two‐body Lippmann‐Schwinger equations have been solved by retaining e+$$ {\mathrm{e}}^{+} $$+H(1 s) and p + Ps(1 s) channels to calculate the cross sections (CS) of the electron capture process at intermediate and high incident energies. The effective interaction of the plasma charged particles is modelled by a pseudopotential which is a function of two parameters, namely the plasma screening strength and the de Broglie wavelength. A detailed study is made to explore the changes in the CSs of the above‐mentioned process with respect to the variation in the plasma screening strength and de Broglie wavelength. Significant changes are found to take place, when the screening strength and the de Broglie wavelength are varied. Specifically, the sharp minimum in the differential CS moves toward the forward direction with increasing de Broglie wavelength at a given screening strength.
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source Wiley-Blackwell Read & Publish Collection
subjects Absorption cross sections
Charged particles
De Broglie wavelengths
Electron capture
hydrogen atom
Plasma
positron scattering
pseudopotential
Scattering
Screening
semi‐classical plasma
Wavelength
title Dynamics of electron capture in positron‐hydrogen scattering under dense semi‐classical plasmas
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