Feynman propagator

E284668

The Feynman propagator is a Green’s function in quantum field theory that encodes the amplitude for a particle to propagate between spacetime points with time-ordering built in.

All labels observed (3)

Label Occurrences
Dirac propagator 1
Feynman propagator canonical 1
Feynman propagators 1

How this entity was disambiguated

Statements (48)

Predicate Object
instanceOf Green's function ⓘ
propagator in quantum field theory ⓘ
alsoKnownAs time-ordered propagator ⓘ
appearsIn Yukawa theory ⓘ
linked to: Yukawa meson theory

quantum chromodynamics ⓘ
quantum electrodynamics ⓘ
scalar field theory ⓘ
argumentType spacetime points ⓘ
definedFor free quantum fields ⓘ
interacting quantum fields (as building blocks in perturbation theory) ⓘ
dependsOn choice of gauge for gauge fields ⓘ
mass of the field ⓘ
spacetime separation between points ⓘ
spin of the field ⓘ
describes amplitude for a particle to propagate between spacetime points ⓘ
domain relativistic quantum field theories ⓘ
encodes vacuum expectation value of the time-ordered product of field operators ⓘ
field quantum field theory ⓘ
hasFeature Lorentz invariance for relativistic fields ⓘ
iε prescription in momentum space ⓘ
hasProperty implements causal boundary conditions via time ordering ⓘ
includes contributions from both positive and negative frequency modes ⓘ
time-ordered ⓘ
translation invariance in homogeneous spacetimes ⓘ
isSpecialCaseOf time-ordered n-point Green's functions (for n=2) ⓘ
mathematicalForm vacuum expectation value of T(A_μ(x)A_ν(y)) for gauge fields ⓘ
vacuum expectation value of T(φ(x)φ(y)) for scalar fields ⓘ
vacuum expectation value of T(ψ(x) ψ̄(y)) for fermionic fields ⓘ
namedAfter Richard Feynman ⓘ
relatedConcept operator formalism of quantum field theory ⓘ
path integral formulation of quantum field theory ⓘ
relatedTo advanced Green's function ⓘ
causal propagator ⓘ
retarded Green's function ⓘ
representation momentum-space Green's function ⓘ
position-space Green's function ⓘ
roleIn construction of Feynman rules ⓘ
definition of the S-matrix in perturbation theory ⓘ
satisfies appropriate wave equation for the field under consideration ⓘ
inhomogeneous Klein–Gordon equation for scalar fields ⓘ
usedFor computing correlation functions ⓘ
describing virtual particle exchange ⓘ
evaluating loop integrals in Feynman diagrams ⓘ
usedIn Feynman diagram calculations ⓘ
derivation of effective field theories ⓘ
perturbative quantum field theory ⓘ
renormalization calculations ⓘ
scattering amplitude computations ⓘ

How these facts were elicited

Referenced by (3)

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

LSZ reduction formula → relatedTo → Feynman propagator ⓘ
Dirac Lagrangian → basisFor → Dirac propagator ⓘ
linked to: Feynman propagator
Wightman correlation functions → relatedTo → Feynman propagators ⓘ
linked to: Feynman propagator