2018
DOI: 10.1103/physrevd.97.065011
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Local modular Hamiltonians from the quantum null energy condition

Abstract: The vacuum modular Hamiltonian K of the Rindler wedge in any relativistic quantum field theory is given by the boost generator. Here we investigate the modular Hamiltonian for more general half-spaces which are bounded by an arbitrary smooth cut of a null plane. We derive a formula for the second derivative of the modular Hamiltonian with respect to the coordinates of the cut which schematically reads K 00 ¼ T vv . This formula can be integrated twice to obtain a simple expression for the modular Hamiltonian. … Show more

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Cited by 36 publications
(50 citation statements)
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“…The definition of M differs from the 1+1 case only through an additional transverse integral over d d−2 y. It can be shown [30,31]…”
Section: Higher-dimensional Casementioning
confidence: 99%
“…The definition of M differs from the 1+1 case only through an additional transverse integral over d d−2 y. It can be shown [30,31]…”
Section: Higher-dimensional Casementioning
confidence: 99%
“…In QFT, it is fundamental for the study of relative entropy [17,18] and its many applications to energy and information inequalities [19][20][21]. In the context of the AdS/CFT correspondence, it is instrumental in the program of reconstructing a gravitational bulk from the holographic data [22][23][24][25][26][27][28][29][30][31][32].…”
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%