Faddeev–Popov ghosts
E860357
Grassmann-valued field
anticommuting field
auxiliary field
concept in quantum field theory
ghost field
tool in path integral quantization
Faddeev–Popov ghosts are auxiliary, anticommuting fields introduced in the path integral quantization of non-Abelian gauge theories to correctly account for gauge redundancy and maintain unitarity and renormalizability.
Observed surface forms (1)
| Surface form | Occurrences |
|---|---|
| BRST symmetry | 1 |
Statements (49)
| Predicate | Object |
|---|---|
| instanceOf |
Grassmann-valued field
ⓘ
anticommuting field ⓘ auxiliary field ⓘ concept in quantum field theory ⓘ ghost field ⓘ tool in path integral quantization ⓘ |
| anticommutationProperty | Grassmann-odd ⓘ |
| appearIn |
BRST-invariant Lagrangian
ⓘ
Faddeev–Popov procedure NERFINISHED ⓘ gauge-fixed action ⓘ |
| appearInGauge |
Feynman gauge
NERFINISHED
ⓘ
Landau gauge NERFINISHED ⓘ Rξ gauges ⓘ |
| associatedWith | gauge group generators ⓘ |
| contributeTo | loop corrections ⓘ |
| doNotAppearAs |
asymptotic physical states
ⓘ
external lines in physical S-matrix elements ⓘ |
| enterAs | additional fields in the gauge-fixed Lagrangian ⓘ |
| fieldType | complex scalar Grassmann field ⓘ |
| introducedBy |
Ludvig Faddeev
NERFINISHED
ⓘ
Victor Popov NERFINISHED ⓘ |
| introducedIn | path integral formalism ⓘ |
| introducedInPublication | Faddeev and Popov 1967 paper on gauge fields NERFINISHED ⓘ |
| introducedTo |
correctly account for gauge volume factor
ⓘ
ensure renormalizability ⓘ fix gauge in path integrals ⓘ handle gauge redundancy ⓘ maintain unitarity ⓘ |
| liveIn | adjoint representation of the gauge group ⓘ |
| LorentzTransformationProperty | scalar ⓘ |
| mathematicalRole | represent Faddeev–Popov determinant ⓘ |
| namedAfter |
Ludvig Faddeev
NERFINISHED
ⓘ
Victor Popov NERFINISHED ⓘ |
| notRequiredIn | Abelian gauge theories in simple gauges ⓘ |
| propagateIn | internal lines of Feynman diagrams ⓘ |
| relatedConcept |
BRST symmetry
NERFINISHED
ⓘ
Faddeev–Popov determinant NERFINISHED ⓘ Fadeev–Popov method NERFINISHED ⓘ Slavnov–Taylor identities NERFINISHED ⓘ gauge fixing ⓘ |
| requiredIn | covariant gauge quantization of non-Abelian theories ⓘ |
| roleInGaugeTheories |
cancel unphysical gauge degrees of freedom
ⓘ
ensure consistency of quantization of non-Abelian fields ⓘ preserve gauge invariance at quantum level ⓘ |
| spin | 0 ⓘ |
| statistics | fermionic ⓘ |
| usedIn |
Yang–Mills theory
NERFINISHED
ⓘ
non-Abelian gauge theory ⓘ quantum chromodynamics NERFINISHED ⓘ |
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.
subject surface form:
't Hooft–Veltman gauge
subject surface form:
't Hooft–Veltman gauge
this entity surface form:
BRST symmetry