1976
DOI: 10.1063/1.522898
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On the duality condition for quantum fields

Abstract: A general quantum field theory is considered in which the fields are assumed to be operator-valued tempered distributions. The system of fields may include any number of boson fields and fermion fields. A theorem which relates certain complex Lorentz transformations to the TCP transformation is stated and proved. With reference to this theorem, duality conditions are considered, and it is shown that such conditions hold under various physically reasonable assumptions about the fields. Extensions of the algebra… Show more

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Cited by 542 publications
(710 citation statements)
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“…If, however, the unperturbed background is such that the undeformed entangling surface exhibits rotational symmetry in the transverse space, then this symmetry will be inherent in the path integral representation ofρ 0 . In particular, as shown in [23] (see also [37][38][39][40][41]) in this caseK 0 is identical to the generator of angular evolution around Σ andÛ takes the form…”
Section: Jhep12(2014)179mentioning
confidence: 78%
“…If, however, the unperturbed background is such that the undeformed entangling surface exhibits rotational symmetry in the transverse space, then this symmetry will be inherent in the path integral representation ofρ 0 . In particular, as shown in [23] (see also [37][38][39][40][41]) in this caseK 0 is identical to the generator of angular evolution around Σ andÛ takes the form…”
Section: Jhep12(2014)179mentioning
confidence: 78%
“…This happens at small enough momentum, p z UV 1 and p z IR 1. 8 In this regime we match (3.29) with (3.26) and then obtain the consequence of the IR regularity condition on the UV expansion. This matching procedure was introduced in [52]; see also [53,54].…”
Section: Jhep03(2016)033mentioning
confidence: 99%
“…It is given by a thermal state with respect to boost "time" evolution, at a fixed dimensionless temperature (2π) −1 . Though this is an old result of axiomatic QFT [8], only recently this fact has been used to provide general results for the EE of a planar surface in terms of correlation functions. Rosenhaus and Smolkin [9][10][11][12] proposed a simple way to compute the planar EE perturbing with relevant operators.…”
Section: Jhep03(2016)033mentioning
confidence: 99%
“…They first realized this at a 1965 conference in Baton Rouge 5 , with statistical mechanics of open systems and the role of the KMS property representing the physical side [7]. The study of the relation between modular operator theory and causal localization in LQP started a decade later [19], and its first application consisted in a more profound understanding [20] of the Unruh Gedankenexperiment [21]. The terminology "modular localization" is more recent and marks the beginning of a new constructive strategy in QFT based on the modular aspects of localization of states and algebras [44] [6].…”
Section: A(r) = B(h(r)) a ≡ B(h) = A(r) ⊗ A(r ⊥ )mentioning
confidence: 99%
“…It has been known for a long time that the algebraic structure associated to free fields allows a functorial interpretation in which operator subalgebras of the global algebra B(H) are the functorial images of certain real subspaces of the Wigner space of one-particle wave functions (the famous so-called "second quantization" 19 ), in particular the spacetime localized algebras are the images of localized real subspaces. This means that the issue of localization to some extend can be studied in the simpler form of localized subspaces of the Wigner particle representation space (unitary positive energy representations of the P-group).…”
Section: Modular Localization and Its Thermal Manifestationmentioning
confidence: 99%