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On renormalisation of λϕ<sup>4</sup>field theory in curved space-time. II
64
Citations
7
References
1980
Year
Curved Space-timePhysicsNatural SciencesParticle PhysicsQuantum Field TheoryQuantum Field Theory In Curved SpacetimeConformal Field TheoryExplicit RenormalisationGauge Field TheoryGauge TheoryPhysical AmplitudesField Theory
For pt.I see ibid., vol.13, p.901 (1980). An explicit renormalisation of all second-order physical processes occurring in lambda phi 4 field theory in conformally flat space-time, including vacuum-to-vacuum processes, is performed. Although divergences dependent on the definition of the vacuum state appear in some Feynman diagrams, physical amplitudes obtained by summing all diagrams which contribute to a single physical process are independent of these divergences. Consequently, the theory remains renormalisable in curved space-time, at least to second order in lambda . Renormalisations of the mass m, the coupling constant lambda and the constant xi which couples the field to the Ricci scalar are required to make two- and four-particle creation amplitudes finite.
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