Mesons in Nuclei in the Light-Front Mean Field Approximation and Deep-Inelastic Scattering

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dc.creatorBurkardt, M.
dc.creatorMiller, G. A.
dc.date1998-02-16
dc.date.accessioned2026-07-07T11:36:40Z
dc.date.available2026-07-07T11:36:40Z
dc.descriptionA light-front treatment for the scalar and vector meson momentum distribution functions is developed using a model in which the nucleus is treated a static source of radius $R$. The limit $R\to \infty$ corresponds to infinite nuclear matter. In this limit, the scalar mesons are shown to carry a vanishing momentum fraction of the nuclear plus momentum $k^+$, but the vector mesons carry a significant fraction, all occuring at the experimentally inaccessible value of $k^+=0$. This confirms earlier work. A study of the $R$ dependence for sizes of real nuclei shows that a fraction of the scalar and vector mesons could be observable.
dc.description9 pages, REVTEX
dc.identifierhttps://arxiv.org/abs/nucl-th/9802049
dc.identifierhttp://arxiv.org/abs/nucl-th/9802049
dc.identifierPhys.Rev.C58:2450-2458,1998
dc.identifierdoi:10.1103/PhysRevC.58.2450
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/198997
dc.subjectNuclear Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.titleMesons in Nuclei in the Light-Front Mean Field Approximation and Deep-Inelastic Scattering
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