Yang–Mills–Stueckelberg theories, framing and local breaking of symmetries

Research output: Contribution to journalArticleResearchpeer review

Authors

  • Alexander D. Popov

Research Organisations

View graph of relations

Details

Original languageEnglish
Article number2350035
Number of pages21
JournalReviews in mathematical physics
Volume36
Issue number1
Early online date21 Oct 2023
Publication statusPublished - Feb 2024

Abstract

We consider Yang–Mills theory with a compact structure group G on a Lorentzian 4-manifold M = R×Σ such that gauge transformations become identity on a submanifold S of Σ (framing over S ⊂ Σ). The space S is not necessarily a boundary of Σ and can have dimension k ≤ 3. Framing of gauge bundles over S ⊂ Σ demands introduction of a G-valued function φS with support on S and modification of Yang–Mills equations along R × S ⊂ M. The fields φS parametrize non-equivalent flat connections mapped into each other by a dynamical group GS changing gauge frames over S. It is shown that the charged condensate φS is the Stueckelberg field generating an effective mass of gluons in the domain S of space Σ and keeping them massless outside S. We argue that the local Stueckelberg field φS can be responsible for color confinement. We also briefly discuss local breaking of symmetries in gravity. It is shown that framing of the tangent bundle over a subspace of spacetime makes gravitons massive in this subspace.

Keywords

    Gauge theories, symmetry breaking

ASJC Scopus subject areas

Cite this

Yang–Mills–Stueckelberg theories, framing and local breaking of symmetries. / Popov, Alexander D.
In: Reviews in mathematical physics, Vol. 36, No. 1, 2350035, 02.2024.

Research output: Contribution to journalArticleResearchpeer review

Popov AD. Yang–Mills–Stueckelberg theories, framing and local breaking of symmetries. Reviews in mathematical physics. 2024 Feb;36(1):2350035. Epub 2023 Oct 21. doi: 10.48550/arXiv.2110.00405, 10.1142/S0129055X23500356
Download
@article{615e7931a6634d8ea0b90b0ff4de2a65,
title = "Yang–Mills–Stueckelberg theories, framing and local breaking of symmetries",
abstract = "We consider Yang–Mills theory with a compact structure group G on a Lorentzian 4-manifold M = R×Σ such that gauge transformations become identity on a submanifold S of Σ (framing over S ⊂ Σ). The space S is not necessarily a boundary of Σ and can have dimension k ≤ 3. Framing of gauge bundles over S ⊂ Σ demands introduction of a G-valued function φS with support on S and modification of Yang–Mills equations along R × S ⊂ M. The fields φS parametrize non-equivalent flat connections mapped into each other by a dynamical group GS changing gauge frames over S. It is shown that the charged condensate φS is the Stueckelberg field generating an effective mass of gluons in the domain S of space Σ and keeping them massless outside S. We argue that the local Stueckelberg field φS can be responsible for color confinement. We also briefly discuss local breaking of symmetries in gravity. It is shown that framing of the tangent bundle over a subspace of spacetime makes gravitons massive in this subspace.",
keywords = "Gauge theories, symmetry breaking",
author = "Popov, {Alexander D.}",
note = "This work was supported by the Deutsche Forschungsgemeinschaft grant LE 838/19.",
year = "2024",
month = feb,
doi = "10.48550/arXiv.2110.00405",
language = "English",
volume = "36",
journal = "Reviews in mathematical physics",
issn = "0129-055X",
publisher = "World Scientific Publishing Co. Pte Ltd",
number = "1",

}

Download

TY - JOUR

T1 - Yang–Mills–Stueckelberg theories, framing and local breaking of symmetries

AU - Popov, Alexander D.

N1 - This work was supported by the Deutsche Forschungsgemeinschaft grant LE 838/19.

PY - 2024/2

Y1 - 2024/2

N2 - We consider Yang–Mills theory with a compact structure group G on a Lorentzian 4-manifold M = R×Σ such that gauge transformations become identity on a submanifold S of Σ (framing over S ⊂ Σ). The space S is not necessarily a boundary of Σ and can have dimension k ≤ 3. Framing of gauge bundles over S ⊂ Σ demands introduction of a G-valued function φS with support on S and modification of Yang–Mills equations along R × S ⊂ M. The fields φS parametrize non-equivalent flat connections mapped into each other by a dynamical group GS changing gauge frames over S. It is shown that the charged condensate φS is the Stueckelberg field generating an effective mass of gluons in the domain S of space Σ and keeping them massless outside S. We argue that the local Stueckelberg field φS can be responsible for color confinement. We also briefly discuss local breaking of symmetries in gravity. It is shown that framing of the tangent bundle over a subspace of spacetime makes gravitons massive in this subspace.

AB - We consider Yang–Mills theory with a compact structure group G on a Lorentzian 4-manifold M = R×Σ such that gauge transformations become identity on a submanifold S of Σ (framing over S ⊂ Σ). The space S is not necessarily a boundary of Σ and can have dimension k ≤ 3. Framing of gauge bundles over S ⊂ Σ demands introduction of a G-valued function φS with support on S and modification of Yang–Mills equations along R × S ⊂ M. The fields φS parametrize non-equivalent flat connections mapped into each other by a dynamical group GS changing gauge frames over S. It is shown that the charged condensate φS is the Stueckelberg field generating an effective mass of gluons in the domain S of space Σ and keeping them massless outside S. We argue that the local Stueckelberg field φS can be responsible for color confinement. We also briefly discuss local breaking of symmetries in gravity. It is shown that framing of the tangent bundle over a subspace of spacetime makes gravitons massive in this subspace.

KW - Gauge theories

KW - symmetry breaking

UR - http://www.scopus.com/inward/record.url?scp=85175460642&partnerID=8YFLogxK

U2 - 10.48550/arXiv.2110.00405

DO - 10.48550/arXiv.2110.00405

M3 - Article

AN - SCOPUS:85175460642

VL - 36

JO - Reviews in mathematical physics

JF - Reviews in mathematical physics

SN - 0129-055X

IS - 1

M1 - 2350035

ER -