Feynman integrals
E1347499
UNEXPLORED
Feynman integrals are mathematical expressions in quantum field theory that represent the contributions of different particle interaction histories to physical processes, typically formulated as integrals over momenta associated with Feynman diagrams.
All labels observed (2)
| Label | Occurrences |
|---|---|
| Feynman integrals canonical | 1 |
| Feynman parameters | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T18865174 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
NED1
Entity disambiguation (via context triple)
gpt-5-mini-2025-08-07
Target entity: Feynman integrals Context triple: [Bogoliubov–Parasyuk theorem, concerns, Feynman integrals]
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A.
Feynman diagrams
Feynman diagrams are graphical representations used in quantum field theory to visualize and calculate particle interactions and processes.
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B.
Schwinger–Dyson equations
The Schwinger–Dyson equations are a set of integral equations in quantum field theory that relate correlation functions and encode the full dynamics of a quantum field.
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C.
Feynman path integral
The Feynman path integral is a formulation of quantum mechanics in which a particle’s behavior is described as a sum over all possible paths it can take, each weighted by a phase factor derived from the classical action.
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D.
Slavnov–Taylor identities
Slavnov–Taylor identities are relations in non-Abelian gauge theories that generalize Ward identities, ensuring the consistency and renormalizability of gauge-invariant quantum field theories.
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E.
Renormalization and Galois Theories
Renormalization and Galois Theories is a mathematical physics work that connects the renormalization process in quantum field theory with Galois theory and motives, revealing deep arithmetic and geometric structures underlying quantum phenomena.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
NED2
Entity disambiguation (via description)
gpt-5-mini-2025-08-07
Target entity: Feynman integrals Target entity description: Feynman integrals are mathematical expressions in quantum field theory that represent the contributions of different particle interaction histories to physical processes, typically formulated as integrals over momenta associated with Feynman diagrams.
-
A.
Feynman diagrams
Feynman diagrams are graphical representations used in quantum field theory to visualize and calculate particle interactions and processes.
-
B.
Schwinger–Dyson equations
The Schwinger–Dyson equations are a set of integral equations in quantum field theory that relate correlation functions and encode the full dynamics of a quantum field.
-
C.
Feynman path integral
The Feynman path integral is a formulation of quantum mechanics in which a particle’s behavior is described as a sum over all possible paths it can take, each weighted by a phase factor derived from the classical action.
-
D.
Slavnov–Taylor identities
Slavnov–Taylor identities are relations in non-Abelian gauge theories that generalize Ward identities, ensuring the consistency and renormalizability of gauge-invariant quantum field theories.
-
E.
Renormalization and Galois Theories
Renormalization and Galois Theories is a mathematical physics work that connects the renormalization process in quantum field theory with Galois theory and motives, revealing deep arithmetic and geometric structures underlying quantum phenomena.
- F. None of above. chosen
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.
linked to: Feynman integrals