The Pion-Nucleon Form Factor From QCD Sum Rules

dc.creatorMeissner, Thomas
dc.date1995-06-29
dc.date.accessioned2026-07-07T11:15:24Z
dc.date.available2026-07-07T11:15:24Z
dc.descriptionQCD sum rules are used to calculate the $q^2$ dependence of the $πNN$ coupling $g_{πNN} (q^2)$ in the spacelike region $0.5 \ {\mbox{GeV}}^2 \lesssim q^2 \lesssim 1.5\ {\mbox{GeV}}^2$. We study the Borel sum rule for the three point function of one pseudoscalar and two nucleon currents up to order four in the operator product expansion. The Borel transform is performed with respect to the nucleon momenta, whereas the momentum $q^2$ of the pseudoscalar vertex is kept fixed at spacelike values. The results can be well fitted using a monopole form with a cutoff mass of about $Λ_π\approx 800 \ {\mbox{MeV}}.
dc.description13 pages (REVTEX), 6 figures as 5 postscript files (as fig.uu tarred, compressed, uudecoded)
dc.identifierhttps://arxiv.org/abs/nucl-th/9506030
dc.identifierhttp://arxiv.org/abs/nucl-th/9506030
dc.identifierPhys.Rev.C52:3386-3392,1995
dc.identifierdoi:10.1103/PhysRevC.52.3386
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/192374
dc.subjectNuclear Theory
dc.subjectHigh Energy Physics - Phenomenology
dc.titleThe Pion-Nucleon Form Factor From QCD Sum Rules
dc.typetext

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