The Pion-Nucleon Form Factor From QCD Sum Rules
Abstract
Description
QCD 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}}.
13 pages (REVTEX), 6 figures as 5 postscript files (as fig.uu tarred, compressed, uudecoded)
13 pages (REVTEX), 6 figures as 5 postscript files (as fig.uu tarred, compressed, uudecoded)