Gell-Mann–Low theorem
E59631
The Gell-Mann–Low theorem is a fundamental result in quantum field theory that rigorously connects interacting quantum fields to free fields via the adiabatic switching-on of interactions, underpinning the use of perturbation theory and the Dyson series.
All labels observed (2)
| Label | Occurrences |
|---|---|
| Gell-Mann–Low theorem canonical | 2 |
| Gell-Mann–Low renormalization group equation | 1 |
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf | theorem in quantum field theory ⓘ |
| appliesTo |
Heisenberg operator formulation of quantum mechanics
ⓘ
surface form:
Heisenberg picture fields
interaction picture fields ⓘ |
| assumes |
existence of adiabatic limit
ⓘ
stability of the vacuum under adiabatic switching ⓘ unique interacting vacuum state ⓘ |
| category | theorem in mathematical physics ⓘ |
| clarifies |
relation between bare and interacting fields
ⓘ
role of interaction picture in QFT ⓘ |
| concerns |
time evolution with switched-on interaction Hamiltonian
ⓘ
vacuum expectation values of time-ordered products ⓘ |
| connects | time-ordered correlation functions of interacting fields to free-field ones ⓘ |
| context | renormalized perturbation theory ⓘ |
| field | quantum field theory ⓘ |
| formalism | operator formalism of quantum field theory ⓘ |
| hasConsequence |
expression of interacting Green’s functions via functional derivatives of generating functional
ⓘ
justification of perturbative expansion around free theory ⓘ |
| historicalContext | developed in early years of renormalized quantum field theory ⓘ |
| implies |
Dyson’s proof of equivalence of Feynman and Schwinger–Tomonaga formulations of QED
ⓘ
surface form:
Dyson series expansion for the S-matrix
|
| importance | fundamental result for the foundations of perturbative QFT ⓘ |
| involves |
S-matrix
ⓘ
time-ordered exponentials ⓘ vacuum-to-vacuum transition amplitudes ⓘ |
| mathematicalFormulation | expresses interacting vacuum as limit of time-evolution operator acting on free vacuum ⓘ |
| namedAfter |
Francis E. Low
ⓘ
Murray Gell-Mann ⓘ |
| provides | rigorous connection between interacting and free fields ⓘ |
| relatedTo |
Dyson’s formula
ⓘ
LSZ reduction formula ⓘ interaction picture time-evolution operator ⓘ renormalization theory ⓘ |
| relates |
free (bare) vacuum state
ⓘ
free quantum fields ⓘ interacting quantum fields ⓘ interacting vacuum state ⓘ |
| requires | adiabatic factor e^{-\epsilon |t|} in interaction Hamiltonian ⓘ |
| underpins |
Dyson series
ⓘ
perturbation theory in quantum field theory ⓘ |
| usedBy | quantum field theorists ⓘ |
| usedFor |
calculation of correlation functions
ⓘ
construction of perturbative expansions ⓘ definition of Green’s functions ⓘ derivation of Feynman rules ⓘ |
| usedIn |
perturbative calculations in particle physics
ⓘ
relativistic quantum field theory ⓘ scattering theory ⓘ |
| usesConcept | adiabatic switching of interactions ⓘ |
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
Gell-Mann–Low renormalization group equation