2008
DOI: 10.1007/s00220-008-0670-7
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The Time Slice Axiom in Perturbative Quantum Field Theory on Globally Hyperbolic Spacetimes

Abstract: The time slice axiom states that the observables which can be measured within an arbitrarily small time interval suffice to predict all other observables. While well known for free field theories where the validity of the time slice axiom is an immediate consequence of the field equation it was not known whether it also holds in generic interacting theories, the only exception being certain superrenormalizable models in 2 dimensions. In this paper we prove that the time slice axiom holds at least for scalar fi… Show more

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Cited by 47 publications
(82 citation statements)
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References 21 publications
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“…Our general argument shows that the association of a cobordism between two Cauchy surfaces of globally hyperbolic spacetimes to an isomorphism of algebras always exists provided the time slice axiom is satisfied. As recently shown, the latter axiom is actually generally valid in perturbative Algebraic Quantum Field Theory [13].…”
Section: Locally Covariant Field Theorymentioning
confidence: 82%
“…Our general argument shows that the association of a cobordism between two Cauchy surfaces of globally hyperbolic spacetimes to an isomorphism of algebras always exists provided the time slice axiom is satisfied. As recently shown, the latter axiom is actually generally valid in perturbative Algebraic Quantum Field Theory [13].…”
Section: Locally Covariant Field Theorymentioning
confidence: 82%
“…In either case the idea is to show that the algebra generated by local operators on a time-slice acts irreducibly on the Hilbert space; the statement then follows from Schur's lemma. In the continuum this idea is called the "time-slice axiom" [3,4]; for recent rigorous discussions, see, e.g., [5,6]. There are actually topological theories where the time-slice axiom is false, for example in Chern-Simons theory quantized on a topologically nontrivial Riemann surface, but we don't expect this loophole to be relevant for CFTs with ordinary gravity duals.…”
Section: Jhep04(2015)163mentioning
confidence: 99%
“…We can fix this ambiguity by fixing the expectation value for any given but fixed m = m 0 , L = L 0 . If one is considering a scalar field of mass m 0 , the usual choice of c 2 would be c 2 = log m 2 0 /16π 2 , so that 20 lim L→∞ ω 0 (φ 2 ) = 0. Once c 2 has been chosen, the expectation value of φ 2 is uniquely determined for any other m, L, and in fact for any other state, such as a finite temperature state.…”
Section: Construction Of Nonlinear Observables For a Free Quantum Scamentioning
confidence: 99%