2000
DOI: 10.1142/s0129055x00000162
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Looking Beyond the Thermal Horizon: Hidden Symmetries in Chiral Models

Abstract: In thermal states of chiral theories, as recently investigated by H.-J. Borchers and J. Yngvason, there exists a rich group of hidden symmetries. Here we show that this leads to a radical converse of of the Hawking-Unruh observation in the following sense. The algebraic commutant of the algebra associated with a (heat bath) thermal chiral system can be used to reprocess the thermal system into a ground state system on a larger algebra with a larger localization space-time. This happens in such a way that the o… Show more

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Cited by 23 publications
(51 citation statements)
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“…In that paper we show that, in fact, a suitable and natural enlargement in the Fock space of the hidden SL ( Essentially speaking, this is due to the behavior of n-point functions on the Killing horizon which is not Hadamard. In this context it would be interesting to investigate the holographic meaning of the Hadamard states (Minkowski vacuum and Hartle-Hawking state) also to make contact with results found in [15,16,17,18] where the net of Von Neumann algebras are defined with respect to Hadamard states.…”
Section: Sl(2 R) Unitary Representations On the Horizon Consider Qfmentioning
confidence: 88%
“…In that paper we show that, in fact, a suitable and natural enlargement in the Fock space of the hidden SL ( Essentially speaking, this is due to the behavior of n-point functions on the Killing horizon which is not Hadamard. In this context it would be interesting to investigate the holographic meaning of the Hadamard states (Minkowski vacuum and Hartle-Hawking state) also to make contact with results found in [15,16,17,18] where the net of Von Neumann algebras are defined with respect to Hadamard states.…”
Section: Sl(2 R) Unitary Representations On the Horizon Consider Qfmentioning
confidence: 88%
“…fluctuations in a small subinterval of a chiral QFT restricted to a halfline, is isomorphic to Einstein's Gedankenexperiment of thermal fluctuations in a heat bath thermodynamic limit state on a line restricted to an interval. Such a tight relation, also referred to a an inverse Unruh effect [24], can not be expected in higher spacetime dimension. Although the thermal aspect of a restricted vacuum in QFT is a structural consequence of causal localization, the general identification of the dimensionless modular temperature with an actual temperature of a heat bath system, or, which is equivalent, the modular "time" with the physical time is not correct; the modular Hamiltonian is does not describe the inertial time for which the local temperature defined in terms of the zeroth thermodynamic law agrees with the "Carnot temperature" of the second law [48].…”
Section: Theorem 1 ([24])mentioning
confidence: 99%
“…In fact in the special case of Jordan's chiral current model (the historically first and simplest model of a QFT), the solution of the E-J conundrum amounts to a unitary isomorphism between a system defined by the vacuum state restricted to the algebra A(I) localized in an interval I and an associated global statistical mechanics system at finite temperature. Such isomorphic relations are referred to as describing an "inverse Unruh effect", [24] and the Jordan model is the only known illustration. However in both cases the KMS temperature is not something which one can measure with a thermometer or use for "eggboiling" 6 (and there is also no "boiling soup" of particle/anti-particle pairs) since the acceleration only affects the "Carnot-temperature" [48].…”
Section: A(r) = B(h(r)) a ≡ B(h) = A(r) ⊗ A(r ⊥ )mentioning
confidence: 99%
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