Equivalence between the gauge \(n\cdot\partial n\cdot A = 0\) and the axial gauge

DOI10.1016/j.nuclphysb.2022.115813zbMath1497.81073arXiv1705.06482OpenAlexW4225281569MaRDI QIDQ2144915

Xin Zhang, Gao-Liang Zhou, Zheng-Xin Yan

Publication date: 17 June 2022

Published in: Nuclear Physics. B (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/1705.06482

Mathematics Subject Classification ID

Operations with distributions and generalized functions (46F10) Perturbations in context of PDEs (35B20) Yang-Mills and other gauge theories in mechanics of particles and systems (70S15) Applications of functional analysis to differential and integral equations (46N20) Canonical quantization (81S08)

Cites Work

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• Field-dependent BRST transformations in Yang-Mills theory
• Gribov horizon beyond the Landau gauge
• Every gauge orbit passes inside the Gribov horizon
• Some remarks on the Gribov ambiguity
• The continuity of the gauge fixing condition \(n \cdot \partial n \cdot A=0\)
• Quantization of Yang-Mills theory without the Gribov ambiguity
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• An all-order proof of the equivalence between Gribov's no-pole and Zwanziger's horizon conditions
• Aspects of the refined Gribov-Zwanziger action in linear covariant gauges
• Finite-Temperature Field Theory
• The Gribov horizon and ghost interactions in Euclidean gauge theories
• Effective action for composite operators
• Study of the properties of the Gribov region inSU(N) Euclidean Yang–Mills theories in the maximal Abelian gauge
• Aspects of Quark Confinement
• Study of the nonlocal gauge invariant mass operator Tr∫d⁴xF_μν(D²)⁻¹F_μνin the maximal Abelian gauge
• Theory of Superconductivity

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