Baryon Self-Energy With QQQ Bethe-Salpeter Dynamics In The Non-Perturbative QCD Regime: n-p Mass Difference
A.N. Mitra

TL;DR
This paper develops a non-perturbative QCD framework using Bethe-Salpeter equations to calculate baryon self-energy and the neutron-proton mass difference, incorporating quark mass differences and electromagnetic effects.
Contribution
It introduces a 3-body Bethe-Salpeter formalism for baryons based on Dyson-Schwinger equations, extending previous 2-body results to accurately compute mass differences.
Findings
Neutron-proton mass difference calculated as just above 1 MeV.
Dominant contribution from d-u quark mass difference (+1.71 MeV).
Electromagnetic effects offset the strong contribution by -0.44 MeV.
Abstract
A qqq BSE formalism based on DB{\chi}S of an input 4-fermion Lagrangian of `current' u,d quarks interacting pairwise via gluon-exchange-propagator in its {\it non-perturbative} regime, is employed for the calculation of baryon self-energy via quark-loop integrals. To that end the baryon-qqq vertex function is derived under Covariant Instantaneity Ansatz (CIA), using Green's function techniques. This is a 3-body extension of an earlier q{\bar q} (2-body) result on the exact 3D-4D interconnection for the respective BS wave functions under 3D kernel support, precalibrated to both q{\bar q} and qqq spectra plus other observables. The quark loop integrals for the neutron (n) - proton (p) mass difference receive contributions from : i) the strong SU(2) effect arising from the d-u mass difference (4 MeV); ii) the e.m. effect of the respective quark charges. The resultant n-p difference comes…
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