2017
DOI: 10.1088/1751-8121/aa7eaa
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Modular Hamiltonians on the null plane and the Markov property of the vacuum state

Abstract: We compute the modular Hamiltonians of regions having the future horizon lying on a null plane. For a CFT this is equivalent to regions with boundary of arbitrary shape lying on the null cone. These Hamiltonians have a local expression on the horizon formed by integrals of the stress tensor. We prove this result in two different ways, and show that the modular Hamiltonians of these regions form an infinite dimensional Lie algebra. The corresponding group of unitary transformations moves the fields on the null … Show more

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Cited by 142 publications
(272 citation statements)
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References 51 publications
(116 reference statements)
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“…In general it is not possible to saturate SSA in the vacuum of a QFT – this is a consequence of the Reeh‐Schlieder theorem. However, one can achieve this when the spatial regions defining the subsystems lie on a null plane . If SSA is saturated for a certain choice of configuration, the density matrix is a quantum Markov state, implying again the structure for ρscriptAscriptC.…”
Section: Discussionmentioning
confidence: 99%
“…In general it is not possible to saturate SSA in the vacuum of a QFT – this is a consequence of the Reeh‐Schlieder theorem. However, one can achieve this when the spatial regions defining the subsystems lie on a null plane . If SSA is saturated for a certain choice of configuration, the density matrix is a quantum Markov state, implying again the structure for ρscriptAscriptC.…”
Section: Discussionmentioning
confidence: 99%
“…Similarly, the stronger statement of non‐negativity of the conditional mutual information, known as strong subadditivity (SSA), is satisfied by all classical probability distributions and quantum density matrices. Since one can think of this property as the monotonicity of correlations under inclusion, its saturation implies a Markov property of the subsystems …”
Section: Introductionmentioning
confidence: 99%
“…Since one can think of this property as the monotonicity of correlations under inclusion, its saturation implies a Markov property of the subsystems. [5,6] However, not all interesting information quantities obey universal bounds: some may satisfy certain inequalities only in one can alternately work directly with the local algebra of observables, thereby circumventing the notion of partitioning of the Hilbert space (which strictly-speaking does not apply). 2 Relative entropy is another quantity which is both finite and meaningful in QFTs.…”
Section: Introductionmentioning
confidence: 99%
“…In shock-wave collisions, QNEC is never saturated in the hydrodynamic regime, but it is saturated in the far-fromequilibrium region, regardless of whether NEC is valid. Reference [40] (see also [41]) conjectures that saturation of QNEC can lead to a simplified expression for (part of) the modular Hamiltonian of a half-space in vacuum. …”
Section: Discussionmentioning
confidence: 99%