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A covariant holographic entanglement entropy proposal
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“The Ryu-Takayanagi formula, including quantum corrections, states that entanglement entropy of the boundary region B is equal to the generalised entropy of the Ryu-Takayanagi surface.”
From Entanglement wedge reconstruction and the information paradox (2020) · cites this paper as [28]
Experimental — accuracy not yet measuredThe source backs part of the claim, not all of it — or backs it for a different population, condition or comparison.
In the citing paper
“In this way, we obtain the quantum extremal surface prescription of [23], and also [20, 21].”
From Replica wormholes and the entropy of Hawking radiation (2020) · cites this paper as [21]
Experimental — accuracy not yet measuredThe source backs part of the claim, not all of it — or backs it for a different population, condition or comparison.
In the citing paper
“The entropy of the black hole is given by the generalized entropy of the quantum extremal surface (QES) [23], which is a quantum-corrected Ryu-Takayanagi (or Hubeny-Rangamani-Takayanagi) surface [20, 21].”
From Replica wormholes and the entropy of Hawking radiation (2020) · cites this paper as [21]
Experimental — accuracy not yet measuredThe source backs part of the claim, not all of it — or backs it for a different population, condition or comparison.
In the citing paper
“The QRT prescription for entanglement entropy between A and ¯ A , or in this case the entanglement entropy between the black hole and the Hawking radiation, is then given by the smallest extremal value of (2.1).”
From Page curve for an evaporating black hole (2020) · cites this paper as [8]
Experimental — accuracy not yet measuredThe source backs part of the claim, not all of it — or backs it for a different population, condition or comparison.
In the citing paper
“This can be explicitly checked with the Ryu-Takayanagi (RT) or the covariant Hubeny-Rangamani-Takayanagi prescription (Ryu and Takayanagi, 2006a,b;Hubeny et al., 2007): The entanglement entropy of a spacelike region A in the CFT is computed in the bulk by the area of a codimension-two minimal surface with boundary anchored on ∂A.”
From Euclidean Wormholes, Baby Universes, and Their Impact on Particle Physics and Cosmology (2018) · cites this paper as Hubeny et al., 2007
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In the citing paper
“Furthermore, since the CFT 2 has a holographic dual, the contribution of the χ fields to the entropy can be computed to leading order using the RT/HRT formula [5,6].”
From The Page curve of Hawking radiation from semiclassical geometry (2020) · cites this paper as [6]
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“In this case, the quantum extremal surface prescription of [7] reduces to the usual RT/HRT [5,6] prescription in the bulk geometry.”
From The Page curve of Hawking radiation from semiclassical geometry (2020) · cites this paper as [6]
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“The RT/HRT formula states that the entanglement entropy of a subregion R of the boundary theory is proportional to the area of the classical, bulk co-dimension two 3extremal surface that is anchored to the boundary of R and is homologous to R (see Fig. 2).”
From Holographic spacetime, black holes and quantum error correcting codes: a review (2022) · cites this paper as [24]
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In the citing paper
“In such a theory, finding quantum extremal surfaces becomes equivalent to finding the RT/HRT surfaces in the higher-dimensional theory.”
From The Page curve of Hawking radiation from semiclassical geometry (2020) · cites this paper as [6]
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Citations
Cites
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“In string theory a natural realization of the holographic principle is manifested by the AdS/CFT correspondence [18, 19] which gives us a precise map between a quantum gravity theory on an asymptotically AdS spacetime M and an ordinary QFT on the conformal boundary ∂M of M.”
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“to the bulk-boundary relation within the AdS/CFT context in § 4. In § 5 we illustrate the calculations of the entanglement entropy using our covariant proposal and demonstrate the consistent agreement with the minimal surface prescri pt ion of [24, 10].”
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“Roughly speaking, the holographic principle states that the number of degrees of freedom in a quantum theory of gravity scales with the area of the system, in contrast to standard QFTs where the entropy is extensive and scales with the volume [15, 16, 17].”
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Entanglement in Quantum Critical Phenomena
Vidal, G., Latorre, J. I., Rico, E., & Kitaev, A. (2003) · Physical Review Letters · doi:10.1103/physrevlett.90.227902 · Cited by 2,793 · cited 1×
“Recently, entanglement entropies of various 1+1 and 2+1 dimensional condensed matter systems have been actively investigated in order to understand zero temperature quantum phase transitions [11, 4, 12, 13, 14].”
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Method
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Sorted by citations
Items 201–300 of 1,007
Geometric aspects of holographic bit threads
Agón, C. A., Jan De Boer, A., & Pedraza, J. F. (2019) · Journal of High Energy Physics · doi:10.1007/jhep05(2019)075 · Cited by 99
“In dynamical situations, however, one needs to upgrade the recipe and use the covariant HRRT formula instead [3].”
BackgroundMethodHolographic tensor network models and quantum error correction: a topical review
Jahn, A., & Eisert, J. (2021) · Quantum Science and Technology · doi:10.1088/2058-9565/ac0293 · Cited by 123
Strongly coupled gauge theories: high and low temperature behavior of non-local observables
Fischler, W., & Kundu, S. (2013) · Journal of High Energy Physics · doi:10.1007/jhep05(2013)098 · Cited by 96
“A precise prescription for computing entanglement entropy for strongly coupled field theories with AdS duals was proposed in [31] and later generalized in [32] (for a good review see [33]).”
BackgroundEntanglement wedge reconstruction and entanglement of purification
Espíndola, R., Güijosa, A., & Pedraza, J. F. (2018) · The European Physical Journal C · doi:10.1140/epjc/s10052-018-6140-2 · Cited by 97
“11 Here we will no longer assume that the geometry is static, so EA is now constructed with the Hubeny–Rangamani–Takayanagi [6] surface associated with A, which we will still denote A.”
BackgroundInfluentialSimple holographic models of black hole evaporation
Akers, C., Engelhardt, N., & Harlow, D. (2020) · Journal of High Energy Physics · doi:10.1007/jhep08(2020)032 · Cited by 121
“where γ is the quantum extremal surface of smallest generalized entropy [8, 15–17], there is some freedom in whether we view their microstates as contributing to the area term or the bulk entropy term.”
BackgroundComments on entanglement negativity in holographic field theories
Rangamani, M., & Rota, M. (2014) · Journal of High Energy Physics · doi:10.1007/jhep10(2014)060 · Cited by 107
“Indeed, the geometrization of the notions of entanglement entropy in the gauge/gravity context for holographic field theories as originally proposed in [9, 10] (and made geometrically covariant in [11]) makes one wonder if there are further (1)LOCC for two parties consists of steps in each of which any party is allowe…”
BackgroundSelf-citationAdS3 holography for 1/4 and 1/8 BPS geometries
Stefano Giusto, B., Moscato, E., & Russo, R. (2015) · Journal of High Energy Physics · doi:10.1007/jhep11(2015)004 · Cited by 98
“If only chiral primary operators (and their descendants) are kept in this expansion, the resulting EE coincides with the one evaluated at the gravity point in the CFT moduli space, which, on the other hand, can be holographically computed via the Ryu-Takayanagi formula [17] (and its generalizations [20]).”
BackgroundMethodInfluentialHolographic complexity equals which action?
Goto, K., Marrochio, H., Myers, R. C., Queimada, L., & Yoshida, B. (2019) · Journal of High Energy Physics · doi:10.1007/jhep02(2019)160 · Cited by 121
Holographic entanglement entropy and gravitational anomalies
Castro, A., Detournay, S., Iqbal, N., & Perlmutter, E. (2014) · Journal of High Energy Physics · doi:10.1007/jhep07(2014)114 · Cited by 99
Evaporating black holes coupled to a thermal bath
Chen, H. Z., Fisher, Z., Hernandez, J., Myers, R. C., & Ruan, S.-M. (2021) · Journal of High Energy Physics · doi:10.1007/jhep01(2021)065 · Cited by 99
“One can study the entropy of the black hole or its complementary subsystem (containing the Hawking radiation) as a function of time, using the Engelhardt-Wall prescription [11] (see also [12]) for calculating von Neumann entropy — a generalization of the Hubeny-Ryu-Rangamani-Takayanagi (HRT) prescription [13, 14] to i…”
MethodDynamical entanglement entropy with angular momentum and U(1) charge
Caputa, P., Mandal, G., & Sinha, R. (2013) · Journal of High Energy Physics · doi:10.1007/jhep11(2013)052 · Cited by 92
“1), the increase EE of a single interval of length l [23] is given by”
BackgroundMethodInfluentialGeneralized entropy for general subregions in quantum gravity
Jensen, K., Sorce, J., & Speranza, A. J. (2023) · Journal of High Energy Physics · doi:10.1007/jhep12(2023)020 · Cited by 151
Strong subadditivity and the covariant holographic entanglement entropy formula
Callan, R., He, J., & Headrick, M. (2012) · Journal of High Energy Physics · doi:10.1007/jhep06(2012)081 · Cited by 90
“It was shown in [4] that the HRT formula, applied to the BTZ spacetime, reproduces (4.”
BackgroundMethodInfluentialBalasubramanian, V., Bernamonti, A., Copland, N. B., Craps, B., & Galli, F. (2011) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.84.105017 · Cited by 106
Holographic holes and differential entropy
Headrick, M., Myers, R. C., & Wien, J. (2014) · Journal of High Energy Physics · doi:10.1007/jhep10(2014)149 · Cited by 89
“Holographic entanglement entropy was first considered in dynamical situations by Hubeny, Rangamani, and Takayanagi (HRT) [17].”
BackgroundInfluentialEvolution of complexity following a global quench
Moosa, M. (2018) · Journal of High Energy Physics · doi:10.1007/jhep03(2018)031 · Cited by 96
“However, it is known [21, 27, 28] that there can be discontinuities in the position of the HRT surface [46], and consequently in the entanglement wedge, when the time t is of the order of the size of the boundary subregion.”
BackgroundBeyond toy models: distilling tensor networks in full AdS/CFT
Bao, N., Penington, G., Sorce, J., & Wall, A. C. (2019) · Journal of High Energy Physics · doi:10.1007/jhep11(2019)069 · Cited by 96
“This conjectured correspondence is made precise for static spacetimes by the Ryu-Takayanagi (RT) formula [2, 3], and for dynamical spacetimes by the Hubeny-Rangamani-Takayanagi (HRT) formula [4].”
BackgroundMethodIncluding contributions from entanglement islands to the reflected entropy
Chandrasekaran, V., Miyaji, M., & Rath, P. (2020) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.102.086009 · Cited by 98
Entanglement phase structure of a holographic BCFT in a black hole background
Geng, H., Karch, A., Perez-Pardavila, C., Raju, S., Randall, L., Riojas, M., & Shashi, S. (2022) · Journal of High Energy Physics · doi:10.1007/jhep05(2022)153 · Cited by 89
Replica wormholes for an evaporating 2D black hole
Goto, K., Hartman, T., & Tajdini, A. (2021) · Journal of High Energy Physics · doi:10.1007/jhep04(2021)289 · Cited by 94
Entanglement entropy in higher derivative holography
Bhattacharyya, A., Kaviraj, A., & Sinha, A. (2013) · Journal of High Energy Physics · doi:10.1007/jhep08(2013)012 · Cited by 85
“Fursaev suggested a derivation [11] of the Ryu-Takayanagi (1)A covariant version was proposed in [5].”
BackgroundBoundary states as holographic duals of trivial spacetimes
Miyaji, M., Ryu, S., Takayanagi, T., & Wen, X. (2015) · Journal of High Energy Physics · doi:10.1007/jhep05(2015)152 · Cited by 90
Self-citationConformal field theories are magical
White, C. D., Cao, C., & Swingle, B. G. (2021) · Physical review. B./Physical review. B · doi:10.1103/physrevb.103.075145 · Cited by 132
Bulk emergence and the RG flow of entanglement entropy
Faulkner, T. (2015) · Journal of High Energy Physics · doi:10.1007/jhep05(2015)033 · Cited by 93
“For this we need to develop the replica trick in real times and presumably this will have some bearing on the HRT conjecture [61] for how to generalize Ryu-Takayanagi to real times.”
On the definition of entanglement entropy in lattice gauge theories
Sinya Aoki, A., Iritani, T., Masahiro Nozaki, A., Numasawa, T., Shiba, N., & Tasaki, H. (2015) · Journal of High Energy Physics · doi:10.1007/jhep06(2015)187 · Cited by 90
“Entanglement entropy plays important roles in various fields of quantum physics including string theory [1–16], condensed matter physics [17–22], and the physics of the black hole [23–27].”
BackgroundInformation flow in black hole evaporation
Chen, H. Z., Fisher, Z., Hernandez, J., Myers, R. C., & Ruan, S.-M. (2020) · Journal of High Energy Physics · doi:10.1007/jhep03(2020)152 · Cited by 144
“tion of the CFT to the generalized entropy is calculated by nding extremal HRT surfaces, i.e., geodesics, in the AdS 3 bulk, in accord with the usual prescription for holographic entanglement entropy [39,40]. In general, these geodesics may connect that endpoints of the relevant intervals in the boundary theory, howev…”
MethodThermalization of the spectral function in strongly coupled two dimensional conformal field theories
Balasubramanian, V., Bernamonti, A., Craps, B., Keränen, V., Keski-Vakkuri, E., Müller, B., Lárus Thorlacius, A., & Vanhoof, J. (2013) · Journal of High Energy Physics · doi:10.1007/jhep04(2013)069 · Cited by 85
“One interesting quantity to consider in such studies is the holographic entanglement entropy [8, 9], which was generalized to time-dependent backgrounds in [10], in particular the collapse of a homogeneous massless shell in the AdS space-time, leading to black hole formation in the bulk, which corresponds to thermaliz…”
BackgroundDisrupting entanglement of black holes
Leichenauer, S. (2014) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.90.046009 · Cited by 94
“hat disrupts this mutual information, we will see the wormhole geometry grow longer. The computation of mutual information is made possible by the Ryu-Takayanagi prescription for entanglement entropy [7, 8]. To a region Aon the left asymptotic boundary we associate 3 a minimal surface in the bulk whose boundary coinci…”
MethodDynamical black holes and expanding plasmas
Figueras, P., Hubeny, V. E., Rangamani, M., & Ross, S. F. (2009) · Journal of High Energy Physics · doi:10.1088/1126-6708/2009/04/137 · Cited by 91
“In fact, it has been argued previously in several different contexts [24, 25] that it may be more appropriate to associate the entropy of the CFT configuration to the area of the apparent horizon rather than the event horizon in the bulk dual.”
BackgroundInfluentialSelf-citationThermalization and entanglement following a nonrelativistic holographic quench
Keränen, V., Keski-Vakkuri, E., & Lárus Thorlacius, A. (2012) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.85.026005 · Cited by 96
Canonical energy is quantum Fisher information
Lashkari, N., & Van Raamsdonk, M. (2016) · Journal of High Energy Physics · doi:10.1007/jhep04(2016)153 · Cited by 90
“In the AdS/CFT correspondence [1], the holographic entanglement entropy formula [2, 3] relates the entanglement structure of the CFT with the geometrical structure of the dual spacetime.”
MethodInfluentialFirst Law of Holographic Complexity
Bernamonti, A., Galli, F., Hernandez, J., Myers, R. C., Ruan, S.-M., & Simón, J. (2019) · Physical Review Letters · doi:10.1103/physrevlett.123.081601 · Cited by 87
Pulling out the island with modular flow
Chen, Y. (2020) · Journal of High Energy Physics · doi:10.1007/jhep03(2020)033 · Cited by 88
“As shown in [1, 2], by applying the standard Ryu-Takayanagi (RT) formula [14] with its generalization including time dependence [15] and quantum correction [16, 17], one finds that the minimal quantum extremal surface has a phase transition at the Page time, which then gives the entropy curve for the black hole in acc…”
MethodReplica wormholes for an evaporating 2D black hole
Goto, K. (2023) · OSTI OAI (U.S. Department of Energy Office of Scientific and Technical Information) · doi:10.1007/jhep04%282021%29289 · Cited by 98
Entanglement entropy and higher spin holography in AdS3
Jan De Boer, A., & Jottar, J. I. (2014) · Journal of High Energy Physics · doi:10.1007/jhep04(2014)089 · Cited by 121
Holographic spacetimes as quantum circuits of path-integrations
Tadashi Takayanagi, B. (2018) · Journal of High Energy Physics · doi:10.1007/jhep12(2018)048 · Cited by 95
“In time-dependent backgrounds, the holographic entanglement entropy is given by the extremal surface area [9].”
BackgroundSelf-citationLearning the Alpha-bits of black holes
Hayden, P., & Penington, G. (2019) · Journal of High Energy Physics · doi:10.1007/jhep12(2019)007 · Cited by 125
Engelhardt, N., & Wall, A. C. (2014) · Journal of High Energy Physics · doi:10.1007/jhep03(2014)068 · Cited by 99
“for purposes of holographic entanglement entropy [12, 13]), we can prove the existence of barriers in more circumstances.”
BackgroundMethodQuantum information in holographic duality
Chen, B., Czech, B., & Wang, Z.-Z. (2022) · Reports on Progress in Physics · doi:10.1088/1361-6633/ac51b5 · Cited by 98
Measuring black hole formations by entanglement entropy via coarse-graining
Takayanagi, T., & Ugajin, T. (2010) · Journal of High Energy Physics · doi:10.1007/jhep11(2010)054 · Cited by 84
“We can calculate SA(t) via AdS/CFT by applying the holographic formula proposed in [14], which generalizes the holographic formula in static spacetime found in [13].”
BackgroundMethodInfluentialSelf-citationPath Integral Optimization as Circuit Complexity
Camargo, H. A., Heller, M. P., Jefferson, R., & Knaute, J. (2019) · Physical Review Letters · doi:10.1103/physrevlett.123.011601 · Cited by 77
Entanglement entropy and superselection sectors. Part I. Global symmetries
Casini, H., Huerta, M., Magán, J. M., & Pontello, D. (2020) · Journal of High Energy Physics · doi:10.1007/jhep02(2020)014 · Cited by 93
Holographic subregion complexity under a thermal quench
Chen, B., Li, W.-M., Yang, R.-Q., Zhang, C.-Y., & Zhang, S.-J. (2018) · Journal of High Energy Physics · doi:10.1007/jhep07(2018)034 · Cited by 83
“For a subregion A on the boundary, its holographic entanglement entropy (HEE) is captured by a codimensiontwo bulk surface with vanishing expansion of geodesics [32], i.”
BackgroundA modular toolkit for bulk reconstruction
Faulkner, T., Li, M., & Wang, H. (2019) · Journal of High Energy Physics · doi:10.1007/jhep04(2019)119 · Cited by 86
“Associated to the region A on the boundary there is a bulk region a between A and the associated HRT extremal surface mA [6, 33].”
BackgroundLeading order corrections to the quantum extremal surface prescription
Akers, C., & Penington, G. (2021) · Journal of High Energy Physics · doi:10.1007/jhep04(2021)062 · Cited by 111
General properties of holographic entanglement entropy
Headrick, M. (2014) · Journal of High Energy Physics · doi:10.1007/jhep03(2014)085 · Cited by 84
Islands in charged linear dilaton black holes
Ahn, B., Bak, S.-E., Jeong, H.-S., Keun-young Kim, A., & Sun, Y.-W. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.105.046012 · Cited by 87
“Although this island prescription is first suggested in the context of the holography (or AdS/CFT correspondence) by Ryu and Takayanagi [19] and its further developments [6, 9–11, 16, 20–22], it can be applied to any quantum system coupled to gravity.”
BackgroundEntanglement between two interacting CFTs and generalized holographic entanglement entropy
Mollabashi, A., Shiba, N., & Takayanagi, T. (2014) · Journal of High Energy Physics · doi:10.1007/jhep04(2014)185 · Cited by 84
Self-citationThe entropy of a hole in spacetime
Balasubramanian, V., Chowdhury, B. D., Czech, B., & Jan De Boer, A. (2013) · Journal of High Energy Physics · doi:10.1007/jhep10(2013)220 · Cited by 86
Holographic entanglement contour, bit threads, and the entanglement tsunami
Kudler-Flam, J., MacCormack, I., & Ryu, S. (2019) · Journal of Physics A Mathematical and Theoretical · doi:10.1088/1751-8121/ab2dae · Cited by 89
Entanglement wedge cross section from CFT: dynamics of local operator quench
Kusuki, Y., & Tamaoka, K. (2020) · Journal of High Energy Physics · doi:10.1007/jhep02(2020)017 · Cited by 81
Pure de Sitter space and the island moving back in time
Sybesma, W. (2021) · Classical and Quantum Gravity · doi:10.1088/1361-6382/abff9a · Cited by 98
Thermalization in backgrounds with hyperscaling violating factor
Alishahiha, M., Astaneh, A. F., & Mozaffar, M. R. M. (2014) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.90.046004 · Cited by 88
“2) Of course since the metric is not static one needs to use the covariant proposal for the holographic entanglement entropy [5].”
BackgroundMethodBCFT and Islands in two dimensions
Suzuki, K., & Tadashi Takayanagi, B. (2022) · Journal of High Energy Physics · doi:10.1007/jhep06(2022)095 · Cited by 85
Self-citationNull geodesics, local CFT operators, and AdS/CFT for subregions
Raphael Bousso, A., Freivogel, B., Leichenauer, S., Rosenhaus, V., & Zukowski, C. (2013) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.88.064057 · Cited by 100
“There is no obvious reason that a geometric region on the boundary has to correspond to a geometric region in the bulk, but there are strong arguments for such a subregion duality in certain simple cases [3], and intriguing hints [4–6] that it may be true more generally.”
Holographic definition of points and distances
Czech, B., & Lamprou, L. (2014) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.90.106005 · Cited by 84
“eralization should be guided by the covariant version of the Ryu-Takayanagi proposal [68], which also satisfies the strong subadditivity of entropy [69].”
MethodHolographic inequalities and entanglement of purification
Bao, N., & Halpern, I. F. (2018) · Journal of High Energy Physics · doi:10.1007/jhep03(2018)006 · Cited by 79
“In particular, the holographic formula relating entanglement entropy to bulk area of a boundary homologous minimal surface by Ryu and Takayanagi [3, 4] (later extended to extremal surfaces in the covariant case by [5]) has spurred a great deal of interest, from its ability to constrain what sets of states can be dual…”
BackgroundHolographic Entanglement of Purification from Conformal Field Theories
Caputa, P., Miyaji, M., Takayanagi, T., & Umemoto, K. (2019) · Physical Review Letters · doi:10.1103/physrevlett.122.111601 · Cited by 82
“(14) The holographic EoP is computed from the length of the entanglement wedge cross section ΣminAB in the hyperbolic space ds2 = (dx2 + dz2)/z2, which is a time slice of Poincare AdS3.”
MethodInfluentialSelf-citationHolographic entanglement negativity and replica symmetry breaking
Dong, X., Qi, X.-L., & Walter, M. (2021) · Journal of High Energy Physics · doi:10.1007/jhep06(2021)024 · Cited by 80
Unitarity from a smooth horizon?
Bousso, R., & Tomašević, M. (2020) · Physical Review D · doi:10.1103/physrevd.102.106019 · Cited by 80
“Such surfaces play a central role in the quantum-corrected [20,21] Ryu-Takayanagi (RT) [22]/ Hubeny-Rangamani-Takayanagi [23] prescription, which”
BackgroundComplexity and entanglement for thermofield double states
Chapman, S., Eisert, J., Hackl, L., Heller, M. P., Jefferson, R., Marrochio, H., & Myers, R. C. (2019) · Refubium (Universitätsbibliothek der Freien Universität Berlin) · doi:10.17169/refubium-25515 · Cited by 80
Leading order corrections to the quantum extremal surface prescription
Akers, C., & Penington, G. (2021) · DSpace@MIT (Massachusetts Institute of Technology) · doi:10.1007/jhep04%282021%29062 · Cited by 87
Conditional and multipartite entanglements of purification and holography
Bao, N., & Halpern, I. F. (2019) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.99.046010 · Cited by 89
“Furthermore, perhaps EW surfaces anchored to boundary-anchored HRT surfaces [19] that probe behind the event horizon of black holes formed from collapse [20] have areas which can be calculated both holographically and directly in the boundary field theory, providing a nontrivial check of the smoothness of the region b…”
BackgroundAkal, I., Kusuki, Y., Shiba, N., Tadashi Takayanagi, B., & Wei, Z. (2021) · Classical and Quantum Gravity · doi:10.1088/1361-6382/ac2c1b · Cited by 86
“We can also extend the holographic entanglement entropy [5, 6, 92] to AdS/BCFT setups.”
BackgroundMethodSelf-citationBlack Hole ThermodynamicsPreprint
Carlip, S. (2014) · Cited by 97
Some aspects of entanglement wedge cross-section
Velni, K. B., Mozaffar, M. R. M., & Vahidinia, M. H. (2019) · Journal of High Energy Physics · doi:10.1007/jhep05(2019)200 · Cited by 75
Entanglement between two disjoint universes
Balasubramanian, V., Kar, A., & Ugajin, T. (2021) · Journal of High Energy Physics · doi:10.1007/jhep02(2021)136 · Cited by 82
“r the Renyi entropy of a thermal ensemble in a 2d CFT in the large climit,8 trˆn ;Cx = sinh ˇL(1 x) n ; trˆn vac;Cx = sin ˇ2x L n n= c 12 n 1 n (2.20) 8We use the holographic expressions [4] for thermal Renyi entropies, though we expect that our result to be be unchanged if we pick a dierent sort of CFT (analogous to…”
MethodInfluentialFailure of the split property in gravity and the information paradox
Raju, S. (2022) · Classical and Quantum Gravity · doi:10.1088/1361-6382/ac482b · Cited by 81
Quasi-local energy and microcanonical entropy in two-dimensional nearly de Sitter gravity
Svesko, A., Verheijden, E., Verlinde, E. P., & Visser, M. R. (2022) · Journal of High Energy Physics · doi:10.1007/jhep08(2022)075 · Cited by 77
“The QES formula is a generalization of the (classical) Ryu– Takayanagi formula [34, 35], which says that the von Neumann entropy in quantum gravity SvN(ΣX) of a codimension-1 slice ΣX bounded by a QES X may be computed in the semi-classical approximation using the following extremization prescription”
Methodde Sitter space, extremal surfaces, and time entanglement
Narayan, K. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.126004 · Cited by 100
“Unlike AdS where specifying boundary data fixes the extremization problem, dS extremal surfaces starting at late times on I+ do not return, thus requiring extra data on boundary conditions in the far past.”
BackgroundInfluentialRiemannian and Lorentzian flow-cut theorems
Headrick, M., & Hubeny, V. E. (2018) · Classical and Quantum Gravity · doi:10.1088/1361-6382/aab83c · Cited by 79
“In the context of holographic entanglement entropy, maximal volume slices were initially considered—but ruled out—in [21] as a step in covariantizing the Ryu-Takayanagi proposal.”
MethodSelf-citationEffective entropy of quantum fields coupled with gravity
Dong, X., Qi, X.-L., Shangnan, Z., & Yang, Z. (2020) · Journal of High Energy Physics · doi:10.1007/jhep10(2020)052 · Cited by 97
“The Ryu-Takayanagi (RT) formula [2] and its generalizations [3–5] provide important clues about how the bulk degrees of freedom corresponds to the boundary ones.”
BackgroundEntanglement Entropies of Equilibrated Pure States in Quantum Many-Body Systems and Gravity
Liu, H., & Vardhan, S. (2021) · PRX Quantum · doi:10.1103/prxquantum.2.010344 · Cited by 77
“n Neumann and Renyi entropies of this nal state should satisfy the unitarity constraint (1.2). In holography, the von Neumann entropy S(A) 1 for a subregion Ais found from the area of the HRT surface [63,64]. For a black hole formed from collapse, the HRT surface for A is the same as that for A, and thus the unitarity…”
BackgroundInfluentialIslands for entanglement negativity
Basak, J. K., Basu, D., Malvimat, V., Parihar, H., & Sengupta, G. (2022) · SciPost Physics · doi:10.21468/scipostphys.12.1.003 · Cited by 84
“Although the island formula is applicable to generic spacetimes, it was inspired by the Ryu-Takayanagi (RT)/Hubeny-Rangamani-Takayanagi (HRT) formula for computing the entanglement entropy of a subsystem in a holographic CFTd [34–37], specifically its quantum corrected formula proposed in [41, 42] .”
MethodThe central dogma and cosmological horizons
Shaghoulian, E. (2022) · Journal of High Energy Physics · doi:10.1007/jhep01(2022)132 · Cited by 78
“When we freeze gravity in the interior of a piece of the static patch (and a similar antipodal region), we will show that generalized entropy computations in de Sitter space have a natural quantum extremal surface [7, 33], stemming from the classical extremal surface (the bifurcation surface) [34, 35], which is a mini…”
BackgroundHolographic entanglement entropy for disconnected regions
Hubeny, V. E., & Rangamani, M. (2008) · Journal of High Energy Physics · doi:10.1088/1126-6708/2008/03/006 · Cited by 73
“As discussed in [5], for general non-static situations one needs to replace the minimal surface by an extremal surface in the bulk.”
BackgroundInfluentialSelf-citationModifications to holographic entanglement entropy in warped CFT
Song, W., Wen, Q., & Xu, J. (2017) · Journal of High Energy Physics · doi:10.1007/jhep02(2017)067 · Cited by 77
“This suggests that at least caution should be taken in applying RT (or HRT) proposal for holography beyond AdS/CFT. Generalization to general temperatures can be done by considering the further mapping from BTZ black holes to Poincaré AdS3 [73], and then follow the steps of section 4.3 in the main text, or section 5.…”
BackgroundMethodInfluentialFrom Euclidean sources to Lorentzian spacetimes in holographic conformal field theories
Marolf, D. M., Parrikar, O., Rabideau, C., Rad, A. I., & Mark Van Raamsdonk, B. (2018) · Journal of High Energy Physics · doi:10.1007/jhep06(2018)077 · Cited by 72
“1) in a large class of CFTs, there is always an associated classical geometry (defined to second order in perturbation theory) which captures the entanglement entropies of ball-shaped regions via the Ryu-Takayanagi formula [9, 10] and which satisfies Einstein’s equations perturbatively to second order.”
MethodHolographic thermalization with Lifshitz scaling and hyperscaling violation
Fonda, P., Franti, L., Keränen, V., Keski-Vakkuri, E., Lárus Thorlacius, A., & Erik Tonni, C. (2014) · Journal of High Energy Physics · doi:10.1007/jhep08(2014)051 · Cited by 72
Scrambling time from local perturbations of the eternal BTZ black hole
Caputa, P., Simón, J., Štikonas, A., Tadashi Takayanagi, B., & Watanabe, K. (2015) · Journal of High Energy Physics · doi:10.1007/jhep08(2015)011 · Cited by 83
“Finally, we compute the entanglement entropy and the mutual information using the holographic prescription [28, 29].”
Self-citationMachine learning spatial geometry from entanglement features
You, Y., Yang, Z., & Qi, X.-L. (2018) · Physical review. B./Physical review. B · doi:10.1103/physrevb.97.045153 · Cited by 80
Replica wormhole and information retrieval in the SYK model coupled to Majorana chains
Chen, Y., Qi, X.-L., & Zhang, P. (2020) · Journal of High Energy Physics · doi:10.1007/jhep06(2020)121 · Cited by 81
“The formula was first proposed for stationary asymptotic anti-de-Sitter (AdS) spacetime, and has been subsequently generalized to time-dependent cases, known as the Hubeny-Rangamani-Ryu-Takayanagi (HRRT) formula [6].”
MethodEvolution of complexity following a quantum quench in free field theory
Alves, D. W. F., & Camilo, G. (2018) · Journal of High Energy Physics · doi:10.1007/jhep06(2018)029 · Cited by 73
“In particular, it has recently become a standard term in the high-energy physics vocabulary due mainly to the AdS/CFT correspondence, the Ryu-Takayanagi formula [1] and its generalization [2].”
BackgroundEffective entropy of quantum fields coupled with gravity
Dong, X., Qi, X.-L., Shangnan, Z., & Yang, Z. (2020) · eScholarship (California Digital Library) · doi:10.1007/jhep10%282020%29052 · Cited by 83
Signatures of global symmetry violation in relative entropies and replica wormholes
Chen, Y., & Lin, H. W. (2021) · Journal of High Energy Physics · doi:10.1007/jhep03(2021)040 · Cited by 88
Matsuo, Y. (2021) · Journal of High Energy Physics · doi:10.1007/jhep07(2021)051 · Cited by 77
Defect extremal surface as the holographic counterpart of Island formula
Deng, F., Chu, J., & Zhou, Y. (2021) · Journal of High Energy Physics · doi:10.1007/jhep03(2021)008 · Cited by 72
The price of curiosity: information recovery in de Sitter space
Aalsma, L., & Sybesma, W. (2021) · Journal of High Energy Physics · doi:10.1007/jhep05(2021)291 · Cited by 82
Holographic quantum circuits from splitting/joining local quenches
Shimaji, T., Takayanagi, T., & Wei, Z. (2019) · Journal of High Energy Physics · doi:10.1007/jhep03(2019)165 · Cited by 70
Self-citationHolographic entropy cone for five regions
Hernández-Cuenca, S. (2019) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.100.026004 · Cited by 74
“The Hubeny-Rangamani-Takayanagi (HRT) prescription gives the covariant generalization of RT that applies to arbitrary dynamical spacetimes [7, 8].”
BackgroundProof of a new area law in general relativity
Raphael Bousso, A., & Engelhardt, N. (2015) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.92.044031 · Cited by 85
“[6].”
Probing Hawking radiation through capacity of entanglement
Kawabata, K., Nishioka, T., Okuyama, Y., & Watanabe, K. (2021) · Journal of High Energy Physics · doi:10.1007/jhep05(2021)062 · Cited by 85
“There are numerous extensions of the formula including time-dependent theories [10, 11], quantum corrections [12], and Rényi entropies [13].”
MethodCauchy slice holography: a new AdS/CFT dictionary
Araujo-Regado, G., Khan, R., & Wall, A. C. (2023) · Journal of High Energy Physics · doi:10.1007/jhep03(2023)026 · Cited by 98
“15There is a dynamical version of the holographic entropy, given by [49]: SHRT[R] = min extγArea[γ]/4GN .”
MethodLarge N phase transitions, finite volume, and entanglement entropy
Johnson, C. V. (2014) · Journal of High Energy Physics · doi:10.1007/jhep03(2014)047 · Cited by 71
Complexity Growth Rate in Lovelock Gravity
Cano, P. A., Hennigar, R. A., & Marrochio, H. (2018) · Physical Review Letters · doi:10.1103/physrevlett.121.121602 · Cited by 79
Kudler-Flam, J., Kusuki, Y., & Ryu, S. (2020) · Journal of High Energy Physics · doi:10.1007/jhep04(2020)074 · Cited by 81
Entanglement between two disjoint universes
Balasubramanian, V. (2023) · OSTI OAI (U.S. Department of Energy Office of Scientific and Technical Information) · doi:10.1007/jhep02%282021%29136 · Cited by 82
Holographic Geometry of cMERA for Quantum Quenches and Finite TemperaturePreprint
Mollabashi, A., Naozaki, M., Ryu, S., & Takayanagi, T. (2016) · Cited by 78
Self-citationRenormalized entanglement entropy
Taylor, M., & Woodhead, W. (2016) · Journal of High Energy Physics · doi:10.1007/jhep08(2016)165 · Cited by 67
“It would be interesting to explore real-time holography in the context of entanglement entropy, using the techniques of [29] for the HRT functional [45].”
MethodThe universality of islands outside the horizon
He, S., Sun, Y., Zhao, L., & Zhang, Y.-X. (2022) · Journal of High Energy Physics · doi:10.1007/jhep05(2022)047 · Cited by 76
“The island formula somehow stems from the investigations of the quantum corrections [19–21] of the Ryu-Takayanagi (RT) formula [22, 23].”
Background
Metadata
- Authors
- Hubeny, V. E., Rangamani, M., & Takayanagi, T.
- Affiliations
- Durham University (GB)
- Kyoto University (JP)
- ORCID
- Hubeny, Veronika E
- Venue
- Journal of High Energy Physics
- Published
- 2007-07-23
- Volume
- 2007
- Issue
- 07
- Pages
- 062-062
- ISSN
- 1029-8479 (ISSN-L)
- OpenAlex
- W2157692768
- Cited by
- 1,822
- References
- 50
- Citations by year
- 2026: 79 · 2025: 151 · 2024: 145 · 2023: 183 · 2022: 182 · 2021: 195 · 2020: 179 · 2019: 144 · 2018: 115 · 2017: 91 · 2016: 112 · 2015: 74 · 2014: 73 · 2013: 36 · 2012: 18
- FWCI
- 6.12
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Journal of High Energy Physics (publishedVersion)
- Durham Research Online (Durham University) (acceptedVersion)
- arXiv (Cornell University) (submittedVersion)
- Durham Research Online (Durham University) (submittedVersion, cc-by)
- arXiv (Cornell University)
- Funders
- Japan Society for the Promotion of Science (19GS0219)
- Kavli Institute for Theoretical Physics, University of California, Santa Barbara
- Topics
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Black Holes and Theoretical Physics
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Noncommutative and Quantum Gravity Theories
- Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum Electrodynamics and Casimir Effect
- Keywords
- holographic entanglement entropy, covariant entropy bound, light sheet, AdS/CFT correspondence, Euclidean wormholes
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