Fermi theory of beta decay

E88964

The Fermi theory of beta decay is Enrico Fermi’s pioneering quantum field theory model that explains beta decay as a weak interaction process mediated by a four-fermion contact interaction, laying the groundwork for modern weak interaction theory.


Statements (44)
Predicate Object
instanceOf effective field theory
physical theory
quantum field theory
theory of weak interaction
appliesTo neutron beta decay
nuclear beta decay
approximates low-energy limit of weak interaction
assumes energy and momentum conservation
lepton number conservation
neutrino emission in beta decay
point-like weak interaction
breaksDownAt high energies
describes beta decay
developer Enrico Fermi
explains continuous beta spectrum
existence of neutrino in beta decay
field nuclear physics
particle physics
theoretical physics
framework quantum field theory
historicalPrecursorOf Standard Model weak interaction
electroweak theory
historicalSignificance first quantitative theory of beta decay
foundation of modern weak interaction theory
inspired development of current–current weak interaction models
interactionForm contact interaction
interactionRange short-range
interactionType four-fermion interaction
weak interaction
introducesConcept Fermi coupling constant
LagrangianContains four-fermion current–current term
laterExtendedTo V–A theory
originallyAssumed vector current
predicts beta decay rate
electron energy spectrum in beta decay
selection rules for beta decay
relatedTo Fermi constant
Gamow–Teller theory
V–A theory of weak interaction
symbolOfCoupling G_F
uses Dirac fields for nucleons and leptons
validAt energies much lower than W boson mass
yearProposed 1933
yearPublished 1934

Referenced by (6)
Subject (surface form when different) Predicate
Fermi constant ("low-energy effective weak interaction Lagrangian")
Fermi constant ("Fermi’s beta decay Hamiltonian")
appearsIn
Enrico Fermi
knownFor
Enrico Fermi
notableFor
Fermi theory of beta decay ("V–A theory of weak interaction")
relatedTo
Fermi constant
usedIn

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