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The Metric on the Space of Yang-Mills Configurations

1 Pith paper cite this work, alongside 11 external citations. Polarity classification is still indexing.

1 Pith paper citing it
11 external citations · Pith
abstract

A distance function on the set of physical equivalence classes of Yang-Mills configurations considered by Feynman and by Atiyah, Hitchin and Singer is studied for both the $2+1$ and $3+1$-dimensional Hamiltonians. This set equipped with this distance function is a metric space, and in fact a Riemannian manifold as Singer observed. Furthermore, this manifold is complete. Gauge configurations can be used to parametrize the manifold. The metric tensor without gauge fixing has zero eigenvalues, but is free of ambiguities on the entire manifold. In $2+1$ dimensions the problem of finding the distance from any configuration to a pure gauge configuration is an integrable system of two-dimensional differential equations. A calculus of manifolds with singular metric tensors is developed and the Riemann curvature is calculated using this calculus. The Laplacian on Yang-Mills wave functionals has a slightly different form from that claimed earlier. In $3+1$-dimensions there are field configurations an arbitrarily large distance from a pure gauge configuration with arbitrarily small potential energy. These configurations resemble long-wavelength gluons. Reasons why there nevertheless can be a mass gap in the quantum theory are proposed.

fields

hep-th 1

years

2026 1

verdicts

CONDITIONAL 1

representative citing papers

Birman-Schwinger Formulation of the Faddeev-Popov Zero-Mode Problem

hep-th · 2026-07-15 · conditional · novelty 6.0

The first Gribov horizon of a transverse gauge background equals the first appearance of −1 in the spectrum of a normalized Birman-Schwinger operator, via an inertia-preserving congruence rather than a similarity.

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Showing 1 of 1 citing paper.

  • Birman-Schwinger Formulation of the Faddeev-Popov Zero-Mode Problem hep-th · 2026-07-15 · conditional · none · ref 33 · internal anchor

    The first Gribov horizon of a transverse gauge background equals the first appearance of −1 in the spectrum of a normalized Birman-Schwinger operator, via an inertia-preserving congruence rather than a similarity.