A Light Front Treatment of the Nucleus-Implications for Deep Inelastic Scattering

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dc.creatorMiller, Gerald A.
dc.date1997-02-14
dc.date.accessioned2026-07-07T11:11:05Z
dc.date.available2026-07-07T11:11:05Z
dc.descriptionA light front treatment of the nuclear wave function is developed and applied, using the mean field approximation, to infinite nuclear matter. The nuclear mesons are shown to carry about a third of the nuclear plus momentum, p+; but their momentum distribution has support only at p+ =0, and the mesons do not contribute to nuclear deep inelastic scattering. This zero mode effect occurs because the meson fields are independent of space-time position.
dc.description11 pages, revtex, 1 figure
dc.identifierhttps://arxiv.org/abs/nucl-th/9702036
dc.identifierhttp://arxiv.org/abs/nucl-th/9702036
dc.identifierPhys.Rev.C56:8-11,1997
dc.identifierdoi:10.1103/PhysRevC.56.R8
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/190978
dc.subjectNuclear Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.titleA Light Front Treatment of the Nucleus-Implications for Deep Inelastic Scattering
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