Dyson’s proof of equivalence of Feynman and Schwinger–Tomonaga formulations of QED
E17385
Dyson’s proof of equivalence of Feynman and Schwinger–Tomonaga formulations of QED is a landmark theoretical result that rigorously demonstrated the mathematical consistency and mutual compatibility of different approaches to quantum electrodynamics.
All labels observed (4)
Statements (44)
| Predicate | Object |
|---|---|
| instanceOf |
result in quantum electrodynamics
ⓘ
theoretical physics result ⓘ |
| author | Freeman Dyson ⓘ |
| clarifies |
relationship between Feynman diagrams and operator methods
ⓘ
status of Feynman diagrams as a systematic expansion ⓘ |
| concerns |
covariant formulation of QED
ⓘ
operator formalism in QED ⓘ path-integral inspired Feynman diagram method ⓘ |
| context |
postwar development of relativistic quantum field theory
ⓘ
resolution of infinities in quantum electrodynamics ⓘ |
| demonstratesEquivalenceOf |
Feynman path integral
ⓘ
surface form:
Feynman formulation of QED
Tomonaga–Schwinger equation ⓘ
surface form:
Schwinger–Tomonaga formulation of QED
Tomonaga–Schwinger equation ⓘ
surface form:
Tomonaga–Schwinger formalism
|
| establishes |
mathematical consistency between different QED formulations
ⓘ
mutual compatibility of Feynman and Schwinger–Tomonaga approaches ⓘ |
| field |
quantum electrodynamics
ⓘ
quantum field theory ⓘ |
| historicalPeriod | late 1940s ⓘ |
| influenced |
pedagogical treatments of perturbative QED
ⓘ
subsequent work on axiomatic quantum field theory ⓘ |
| involves |
comparison of S-matrix elements
ⓘ
covariant perturbation expansion ⓘ expansion of the S-matrix in powers of the coupling constant ⓘ time-ordered exponential of the interaction Hamiltonian ⓘ |
| relatedToPerson |
Julian Schwinger
ⓘ
Richard Feynman ⓘ Sin-Itiro Tomonaga ⓘ |
| relatedWork |
S-matrix
ⓘ
surface form:
Dyson’s papers on the S-matrix in quantum electrodynamics
|
| relatesTo |
Feynman diagrams
ⓘ
Tomonaga–Schwinger equation ⓘ covariant commutation relations ⓘ |
| shows |
Feynman rules reproduce Tomonaga–Schwinger operator results order by order
ⓘ
Lorentz invariance of the perturbation expansion can be maintained ⓘ diagrammatic expansion corresponds to time-ordered products of interaction terms ⓘ |
| significance |
contributed to acceptance of Feynman diagram technique
ⓘ
helped unify competing formulations of QED ⓘ landmark result in the development of renormalized QED ⓘ provided rigorous foundation for perturbative QED calculations ⓘ |
| supports | view that different QED formalisms are representations of the same underlying theory ⓘ |
| usesConcept |
Dyson series
ⓘ
S-matrix ⓘ interaction picture ⓘ perturbation theory in QED ⓘ time-ordered products ⓘ |
Referenced by (4)
Full triples — surface form annotated when it differs from this entity's canonical label.
Freeman Dyson
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notableWork
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Dyson’s proof of equivalence of Feynman and Schwinger–Tomonaga formulations of QED
ⓘ
Sin-Itiro Tomonaga
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notableWork
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Dyson’s proof of equivalence of Feynman and Schwinger–Tomonaga formulations of QED
ⓘ
this entity surface form:
Relativistic formulation of quantum field theory
Dyson
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notableWork
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Dyson’s proof of equivalence of Feynman and Schwinger–Tomonaga formulations of QED
ⓘ
subject surface form:
Freeman Dyson
this entity surface form:
Dyson’s formulation of quantum electrodynamics
Gell-Mann–Low theorem
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implies
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Dyson’s proof of equivalence of Feynman and Schwinger–Tomonaga formulations of QED
ⓘ
this entity surface form:
Dyson series expansion for the S-matrix