1996
DOI: 10.1006/aphy.1996.0060
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Nucleon Observables and Loop Diagrams in Cavity QCD

Abstract: Using a technique which is based on dimensional regularization, loop corrections to vertex diagrams of a massless quark moving in a spherical cavity are calculated in an arbitrary covariant gauge. Including the finite one-gluon-exchange diagrams, the corrections to the magnetic moments, vector and axial vector coupling constants, and the various r.m.s. radii of the nucleon are evaluated to order : S .

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Cited by 2 publications
(6 citation statements)
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“…where u n ( x) and a µ mΣ ( x) are the quark and gluon cavity modes, respectively [11]. The result is…”
Section: Second Order Energy Shiftmentioning
confidence: 97%
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“…where u n ( x) and a µ mΣ ( x) are the quark and gluon cavity modes, respectively [11]. The result is…”
Section: Second Order Energy Shiftmentioning
confidence: 97%
“…Here, we have used the quark and gluon propagators in the Feynman gauge [11]. The subscripts of the quark creation and annihilation operators stand for the color, flavor, and orbital quantum numbers, respectively.…”
Section: Second Order Energy Shiftmentioning
confidence: 99%
“…Here the a D,N n,l,µ (x) denote the scalar cavity modes for either Dirichlet or Neumann boundary conditions, and the N D,N n,l stand for their normalization constants [15,24], respectively, as explained in Appendix A.1. Using the plane-wave representation of the free-space propagator implies a z −3 divergence in the free-space part of Eq.…”
Section: Massless Scalar Fieldsmentioning
confidence: 99%
“…Using Eq. ( 8), the mode summation representing the cavity Dirac propagator [15,24], the spherical representation of the free-space propagator, and introducing the Schwinger z-integral, we obtain, after an angular integration, θ00 (r)…”
Section: Massless Dirac Fieldsmentioning
confidence: 99%
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