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.

Try in SPARQL Jump to: Surface forms Statements Referenced by

All labels observed (3)

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

Statements (48)

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

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 Feynman propagator
this entity surface form: Dirac propagator
Wightman correlation functions relatedTo Feynman propagator
this entity surface form: Feynman propagators