The extraction of the axial coupling from finite volume systems: The long and short of it
arXiv:hep-lat/0112014 · doi:10.1016/S0370-2693(02)01241-8
Abstract
Due to a pion-pole contribution, the nucleon axial current matrix elements can be visualized in position space as becoming delocalized as the chiral limit is approached, with one-third of the current at distance of order the inverse pion mass. However, this delocalization effect will not cause calculations of the axial coupling in a finite system with standard boundary conditions (periodic for boson fields, antiperiodic for fermions) to have large finite volume effects. This is seen by calculating axial coupling using a nonstandard current with axial quantum numbers. The matrix elements of this new current lacks a pion pole and is not delocalized; however, its zero-momentum matrix element is identical to that of the standard axial current both for infinite and finite volumes.
6 pages
References in corpus (5)
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Cited by in corpus (12)
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- Time Dependence of Nucleon Correlation Functions in Chiral Perturbation Theory
- Chiral Corrections to Nucleon Two- and Three-Point Correlation Functions
- Quark scalar, axial, and pseudoscalar charges in the Schwinger-Dyson formalism
- Calculation of Moments of Structure Functions
- Detailed analysis of excited state systematics in a lattice QCD calculation of
- Finite Volume Dependence of Hadron Properties and Lattice QCD
- Nucleon axial charge from quenched lattice QCD with domain wall fermions and DBW2 gauge action
- Axial Vector Current and Coupling of the Quark in the Instanton Model