’t Hooft–Veltman gauge

E415090
concept in quantum field theory gauge-fixing scheme renormalizable gauge

The ’t Hooft–Veltman gauge is a renormalizable gauge-fixing scheme in quantum field theory, particularly used in non-Abelian gauge theories to simplify calculations and maintain consistency of the theory.

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All labels observed (2)

Label Occurrences
’t Hooft gauge 1
’t Hooft–Veltman gauge canonical 1

Statements (39)

Predicate Object
instanceOf concept in quantum field theory ⓘ
gauge-fixing scheme ⓘ
renormalizable gauge ⓘ
aimsTo define propagators for gauge fields ⓘ
eliminate gauge redundancy ⓘ
appliesTo Yang–Mills theory ⓘ
surface form: Yang–Mills theories

non-Abelian gauge theories ⓘ
category gauge choice ⓘ
quantization condition for gauge fields ⓘ
compatibleWith Higgs mechanism ⓘ
spontaneously broken gauge symmetry ⓘ
dependsOn gauge parameter ⓘ
gauge-fixing function ⓘ
ensures consistency of the quantum theory ⓘ
renormalizability of non-Abelian gauge theories ⓘ
field quantum field theory ⓘ
formalism Lagrangian formalism ⓘ
path integral quantization ⓘ
hasProperty covariant ⓘ
perturbative ⓘ
renormalizable ⓘ
introducedBy Gerard ’t Hooft ⓘ
Martinus Veltman ⓘ
surface form: Martinus J. G. Veltman
namedAfter Gerard ’t Hooft ⓘ
Martinus Veltman ⓘ
surface form: Martinus J. G. Veltman
relatedTo Faddeev–Popov ghosts ⓘ
surface form: BRST symmetry

Faddeev–Popov ghosts ⓘ
Rξ gauge ⓘ
gauge-fixing Lagrangian ⓘ
’t Hooft–Veltman gauge self-linksurface differs ⓘ
surface form: ’t Hooft gauge
usedFor gauge fixing ⓘ
maintaining renormalizability ⓘ
maintaining unitarity ⓘ
simplifying perturbative calculations ⓘ
usedIn Standard Model calculations ⓘ
Salam–Weinberg model ⓘ
surface form: electroweak theory

loop calculations ⓘ
usedToDerive Feynman rules for gauge bosons ⓘ
Feynman rules for ghost fields ⓘ

Referenced by (2)

Full triples — surface form annotated when it differs from this entity's canonical label.

Gerard ’t Hooft → notableWork → ’t Hooft–Veltman gauge ⓘ
’t Hooft–Veltman gauge → relatedTo → ’t Hooft–Veltman gauge self-linksurface differs ⓘ
subject surface form: 't Hooft–Veltman gauge
this entity surface form: ’t Hooft gauge