Dynamic Screening in Thermonuclear Reactions

dc.creatorOpher, Merav
dc.creatorOpher, Reuven
dc.date1999-08-19
dc.date.accessioned2026-07-07T11:46:10Z
dc.date.available2026-07-07T11:46:10Z
dc.descriptionIt has recently been argued that there are no dynamic screening corrections to Salpeter's enhancement factor in thermonuclear reactions, in the weak-screening limit. The arguments used were: 1) The Gibbs probability distribution is factorable into two parts, one of which, $exp(-β\sum e_{i}e_{j}/r_{ij})$ ($β=1/k_{B}T$), is independent of velocity space; and 2) The enhancement factor is $w=1+β^{2}e^{2}Z_{1}Z_{2}< ϕ^{2} >$ with ${< ϕ^{2} >}_{k}={< E^{2} >}_{k}/k^{2}$ and ${< E^{2} >}_{k}/(8π)=(T/2)[1-ε^{-1} (0,k)]$. We show that both of these arguments are incorrect.
dc.descriptionAccepted for publication in The Astrophysical Journal
dc.identifierhttps://arxiv.org/abs/astro-ph/9908218
dc.identifierhttp://arxiv.org/abs/astro-ph/9908218
dc.identifierAstrophys.J.535:473-474,2000
dc.identifierdoi:10.1086/308808
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/202133
dc.subjectAstrophysics
dc.subjectPlasma Physics
dc.titleDynamic Screening in Thermonuclear Reactions
dc.typetext

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