Reflection-positive continuum reconstruction of SU(N) Yang–Mills theory with a nonzero mass gap: Part (3)

In this paper, we seek order in a hard matter by trusting two guides that do not mislead: positivity and invariance. From a reflection-positive (RP) lattice formulation of SU[Formula: see text] Yang–Mills, choosing on each time slice a definite transverse form and gently damping distant modes, we proceed by steps that preserve these guides. From such simple means we pass to the continuum: Euclidean correlation functions satisfy the Osterwalder–Schrader axioms, and the Wightman theory with a unique vacuum and positive energy follows. The decisive point is the scale: time-correlations are completely monotone and decay uniformly, so the spectral measure cannot touch zero; and along the same flow the vacuum-orthogonal evolution decays at a fixed rate, which survives in the limit. Thus a strictly positive, volume-independent spectral gap is obtained for the continuum Hamiltonian, and the bridge from Euclidean positivity to Hilbert-space dynamics remains intact.

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Publication Details

Journal
International Journal of Geometric Methods in Modern Physics
Published
2026-01-16
DOI
https://doi.org/10.1142/s0219887826501124
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
0.00
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article

Reflection-positive continuum reconstruction of SU(N) Yang–Mills theory with a nonzero mass gap: Part (3)

Arshid Shabir, Mir Faizal
International Journal of Geometric Methods in Modern Physics
Quantum Chromodynamics and Particle Interactions
article

Reflection-positive continuum reconstruction of SU(N) Yang–Mills theory with a nonzero mass gap: Part (3)

Arshid Shabir, Mir Faizal
article en

Abstract

In this paper, we seek order in a hard matter by trusting two guides that do not mislead: positivity and invariance. From a reflection-positive (RP) lattice formulation of SU[Formula: see text] Yang–Mills, choosing on each time slice a definite transverse form and gently damping distant modes, we proceed by steps that preserve these guides. From such simple means we pass to the continuum: Euclidean correlation functions satisfy the Osterwalder–Schrader axioms, and the Wightman theory with a unique vacuum and positive energy follows. The decisive point is the scale: time-correlations are completely monotone and decay uniformly, so the spectral measure cannot touch zero; and along the same flow the vacuum-orthogonal evolution decays at a fixed rate, which survives in the limit. Thus a strictly positive, volume-independent spectral gap is obtained for the continuum Hamiltonian, and the bridge from Euclidean positivity to Hilbert-space dynamics remains intact.

International Journal of Geometric Methods in Modern Physics
Durham University (GB), Canadian Quantum Research Center (CA), Okanagan University College (CA), Hasselt University (BE)
Openalex Percentile: Top 82%
Quantum Chromodynamics and Particle Interactions
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