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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]
The cited source says what the claim attributes to it.
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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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In the citing paper
“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
The large $N$ limit of superconformal field theories and supergravity
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“, GKP-W relation [38, 39] for the AdS/CFT correspondence.”
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“, GKP-W relation [38, 39] for the AdS/CFT correspondence.”
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Large N field theories, string theory and gravity
Ofer Aharony, A., Gubser, S. S., MALDACENA, J. M., Ooguri, H., & Oz, Y. (2000) · Physics Reports · doi:10.1016/s0370-1573(99)00083-6 · Cited by 6,395 · cited 3×
“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.”
BackgroundMethodRyu, S., & Takayanagi, T. (2006) · Physical Review Letters · doi:10.1103/physrevlett.96.181602 · Cited by 4,302 · cited 8×
“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].”
BackgroundMethodInfluentialSelf-citationSusskind, L. (1995) · Journal of Mathematical Physics · doi:10.1063/1.531249 · Cited by 4,085 · cited 1×
“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].”
BackgroundBlack hole in three-dimensional spacetime
Bañados, M., Teitelboim, C., & Zanelli, J. (1992) · Physical Review Letters · doi:10.1103/physrevlett.69.1849 · Cited by 3,831
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].”
BackgroundBrown, J. D., & Henneaux, M. (1986) · Communications in Mathematical Physics · doi:10.1007/bf01211590 · Cited by 2,605 · cited 1×
“Using the relation between the central charge of the dual CFT and the bulk Newton’s constant c = 3 2G (3) N [50], we obtain the expression in the dual CFT language”
Method
Flagged first, then by citations
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Sorted by citations
Items 901–1,000 of 1,007
Path integral complexity and Kasner singularities
Caputa, P., Das, D., & Das, S. R. (2022) · Journal of High Energy Physics · doi:10.1007/jhep01(2022)150 · Cited by 16
“The same general result (8.6) can be simply derived holographically using the HRT [34] prescription in Banados geometries [44].”
BackgroundMethodInfluentialKibe, T., Mukhopadhyay, A., & Roy, P. (2022) · Physical Review Letters · doi:10.1103/physrevlett.128.191602 · Cited by 16
Generalized volume-complexity for two-sided hyperscaling violating black branes
Omidi, F. (2023) · Journal of High Energy Physics · doi:10.1007/jhep01(2023)105 · Cited by 16
“J H E P 0 1 ( 2 0 2 3 ) 1 0 5 It should be pointed out that volume-complexity1 was also introduced for some subregions in the bulk spacetime such as in a region [11, 12] enclosed by a (H)RT hypersurface [13, 14] or inside a Wheeler-DeWitt (WDW) patch [15].”
BackgroundEntanglement from dissipation and holographic interpretation
Cantcheff, M. B., Gadelha, A. L., Marchioro, D. F. Z., & Nedel, D. L. (2018) · The European Physical Journal C · doi:10.1140/epjc/s10052-018-5545-2 · Cited by 16
“The Vaidya solution is the simplest example of a time dependent gravitational background which is explored in the context of the RT conjecture [6,68,69].”
BackgroundDetermining a Riemannian metric from minimal areas
Alexakis, S., Balehowsky, T., & Nachman, A. (2020) · Advances in Mathematics · doi:10.1016/j.aim.2020.107025 · Cited by 16
Bit threads and the membrane theory of entanglement dynamics
Agón, C. A., & Mezei, M. (2021) · Journal of High Energy Physics · doi:10.1007/jhep11(2021)167 · Cited by 23
“The original derivation of the membrane theory relies on the HRT prescription [3] for the computation of the holographic entanglement entropy in dynamical settings.”
MethodBulk geometry from entanglement entropy of CFT
Saha, A., Karar, S., & Gangopadhyay, S. (2020) · The European Physical Journal Plus · doi:10.1140/epjp/s13360-020-00110-7 · Cited by 15
Entanglement measures for nonconformal D-branes
Lala, A. (2020) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.102.126026 · Cited by 14
“Perhaps the most prominent of all these examples is the holographic computations of entanglement entropy of the dual boundary theory of interest which is particularly useful in determining the entanglement entropy of pure states [4, 5, 6, 7, 8].”
BackgroundA holographic study of the characteristics of chaos and correlation in the presence of backreaction
Chakrabortty, S., Hoshino, H., Pant, S., & Sil, K. (2023) · Physics Letters B · doi:10.1016/j.physletb.2023.137749 · Cited by 16
“When γA∪B = γwormhole, the computation of S(A ∪ B) follows from the Hubeny-Rangamani-Takayanagi (HRT) prescription [29] where the determinants of induced metrics corresponding to the extremal surfaces are,”
MethodChaos and fast scrambling delays of a dyonic Kerr-Sen- AdS4 black hole and its ultraspinning version
Prihadi, H. L., Zen, F. P., Dwiputra, D., & Ariwahjoedi, S. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.124053 · Cited by 15
Holographic complexity of Jackiw-Teitelboim gravity from Karch-Randall braneworld
Bhattacharya, A., Bhattacharyya, A., & Patra, A. (2023) · Journal of High Energy Physics · doi:10.1007/jhep07(2023)060 · Cited by 15
“More precisely, the generalized entropy of (II) is well-approximated, to leading order in 1/GN , in (III) by a classical entanglement surface computed via the Ryu-Takayanagi (RT) prescription [91] (or its covariant extension [92]) — the surface is extremal and thus must satisfy appropriate boundary condition on the br…”
BackgroundMethodBoundary-induced transitions in Möbius quenches of holographic BCFT
Bernamonti, A., Galli, F., & Ge, D. (2024) · Journal of High Energy Physics · doi:10.1007/jhep06(2024)184 · Cited by 15
Two infinite families of facets of the holographic entropy cone
Czech, B., Liu, Y., & Yu, B. (2024) · SciPost Physics · doi:10.21468/scipostphys.17.3.084 · Cited by 15
“A cornerstone of this relation is the Ryu-Takayanagi (RT) formula [ 2, 3 ] and its generalizations [ 4–7 ] , which relate extremal areas in spacetime to entanglement entropies of the corresponding quantum state in the holo-graphically dual theory.”
MethodColafranceschi, E., Dong, X., Marolf, D. M., & Wang, Z. (2024) · Journal of High Energy Physics · doi:10.1007/jhep10(2024)063 · Cited by 31
Imaginary part of timelike entanglement entropy
Xu, J., & Guo, W.-Z. (2025) · Journal of High Energy Physics · doi:10.1007/jhep02(2025)094 · Cited by 15
“Intriguingly, within the AdS/CFT framework [7, 8, 9], entanglement entropy has been discovered to correlate with minimal surfaces in the corresponding spacetime [10, 11], adhering to a principle akin to the area law observed in black holes.”
MethodFigueras, P., & Tunyasuvunakool, S. (2014) · Journal of High Energy Physics · doi:10.1007/jhep06(2014)025 · Cited by 15
“Subsequently the proposal of [18, 19] has been generalized to time-dependent situations [20] and, more relevant for this paper, to confining backgrounds [21] (see also [22]).”
BackgroundJurić, T., & Samsarov, A. (2016) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.93.104033 · Cited by 19
Holographic integral geometry with time dependence
Czech, B., Olivas, Y. D., & Wang, Z.-Z. (2020) · Journal of High Energy Physics · doi:10.1007/jhep12(2020)063 · Cited by 15
“In holographic duality, key insights concerning the microscopic fabric of spacetime—the Ryu-Takayanagi proposal [1, 2] with its various reformulations and generalizations [3–5], holographic entropy inequalities [6, 7], error correction [8] or the analogy to tensor networks [9–11]—all stipulate the existence of some pr…”
BackgroundMethodHolographic informational properties for a specific Einstein-Maxwell-dilaton gravity theory
Fu, G., Liu, P., Gong, H., Kuang, X., & Wu, J.-P. (2021) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.104.026016 · Cited by 14
“For covariant cases, RT formula is reformulated into the Hubeny-Rangamani-Takayanagi (HRT) formula [13, 14].”
MethodA Rényi quantum null energy condition: proof for free field theories
Moosa, M., Rath, P., & Su, V. P. (2021) · Journal of High Energy Physics · doi:10.1007/jhep01(2021)064 · Cited by 19
Informational properties of holographic Lifshitz field theory *
Gong, H., Liu, P., Fu, G., Kuang, X., & Wu, J.-P. (2021) · Chinese Physics C · doi:10.1088/1674-1137/abefca · Cited by 14
“Later, RT formula is extended to the covariant case, which is dubbed as the Hubeny-Rangamani-Takayanagi (HRT) formula [8, 9].”
MethodMixed state entanglement and thermal phase transitions
Liu, P., & Wu, J.-P. (2021) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.104.046017 · Cited by 22
“[6] V.”
BackgroundMore of the bulk from extremal area variations
Bao, N., Cao, C., Fischetti, S., Pollack, J., & Zhong, Y. (2020) · Classical and Quantum Gravity · doi:10.1088/1361-6382/abcfd0 · Cited by 13
Reflected entropy for communicating black holes. Part I. Karch-Randall braneworlds
Afrasiar, M., Basak, J. K., Chandra, A., & Sengupta, G. (2023) · Journal of High Energy Physics · doi:10.1007/jhep02(2023)203 · Cited by 16
Scale versus conformal invariance from entanglement entropy
Naseh, A. (2016) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.94.125015 · Cited by 16
All the entropies on the light-cone
Casini, H., Testé, E., & Torroba, G. (2018) · Journal of High Energy Physics · doi:10.1007/jhep05(2018)005 · Cited by 19
“Via the HRT formula [38, 39], this translates into finding extremal surfaces anchored at boundary curves γ(y) in the null surfaces in asymptotically AdS space.”
MethodRestricted Maximin surfaces and HRT in generic black hole spacetimes
Marolf, D., Wall, A. C., & Wang, Z. (2019) · Journal of High Energy Physics · doi:10.1007/jhep05(2019)127 · Cited by 15
“of HRT surfaces in standard charged and rotating black holes6 3 Discussion6 1 Introduction As is by now well established [1,2], in AdS/CFT the Ryu-Takayangi [3,4] and HubenyRangamani-Takayanagi (HRT) [5] prescriptions generally describe the von Neumann entropy of CFT regions Ain terms of the area of an appropriate bul…”
BackgroundInfluentialHolographic entanglement first law for d + 1 dimensional rotating cylindrical black holes
Nadi, H., Mirza, B., Sherkatghanad, Z., & Mirzaiyan, Z. (2019) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2019.114822 · Cited by 15
“The covariant version of the RT proposal for the bulk metric, which is either non-static or even non-stationary, was presented in [6] and the HEE was derived for rotating BTZ black holes as a stationary but non-static spacetime.”
MethodSurface growth scheme for bulk reconstruction and tensor network
Lin, Y.-Y., Sun, J.-R., & Sun, Y. (2020) · Journal of High Energy Physics · doi:10.1007/jhep12(2020)083 · Cited by 15
Restricted Maximin surfaces and HRT in generic black hole spacetimes
Marolf, D. M., Wall, A. C., & Wang, Z. (2019) · eScholarship (California Digital Library) · Cited by 15
Aref’eva, I. Y., & Volovich, I. V. (2013) · Theoretical and Mathematical Physics · doi:10.1007/s11232-013-0016-2 · Cited by 15
Local quenches from a Krylov perspective
Caputa, P., & Giulio, G. D. (2025) · Journal of High Energy Physics · doi:10.1007/jhep07(2025)164 · Cited by 14
Extremal surfaces and entanglement entropy
Pal, S. S. (2014) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2014.03.004 · Cited by 14
Anisotropic flows into black holes
Cáceres, E., & Shashi, S. (2023) · Journal of High Energy Physics · doi:10.1007/jhep01(2023)007 · Cited by 14
Entanglement negativity in T T ¯ -deformed CFT 2 s
Basu, D., Chawla, L., & Paul, B. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.126026 · Cited by 14
“Furthermore, a covariant generalization of this formula was proposed in [11].”
Defect extremal surfaces for entanglement negativity
Basu, D., Parihar, H., Raj, V., & Sengupta, G. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.106005 · Cited by 23
“The lengths of the extremal curves may now be obtained in the un-primed coordinates through the standard Poincar´e AdS 3 result as follows [10,11] (5.16) In the above expression, (cid:15) is the UV cut-off for the original BCFT 2 in the primed coordinates and the second logarithmic term arises due…”
BackgroundMethodInfluentialHolographic complexity of rotating quantum black holes
Chen, B., Liu, Y., & Yu, B. (2024) · Journal of High Energy Physics · doi:10.1007/jhep01(2024)055 · Cited by 14
“A prime example is the holographic entanglement entropy proposed by Ryu-Takayanagi[4, 5], manifesting the idea that geometry is emergent.”
Entanglement and Chaos near critical point in strongly coupled Gauge theory
Karan, D., & Pant, S. (2024) · The European Physical Journal C · doi:10.1140/epjc/s10052-024-12463-9 · Cited by 14
“To find area of γ wormhole we use the prescription given by Hubeny–Rangamani–Takayanagi (HRT) [20].”
Reflected entropy in a BCFT on a black hole background
Basu, D., Chourasiya, H., Raj, V., & Sengupta, G. (2024) · Journal of High Energy Physics · doi:10.1007/jhep05(2024)054 · Cited by 14
“The island formula may then be obtained through the RT prescription [9–11] in the corresponding higher-dimensional bulk perspective.”
BackgroundGeneralized Fefferman-Graham gauge and boundary Weyl structures
Arenas-Henriquez, G., Díaz, F., & Rivera-Betancour, D. (2025) · Journal of High Energy Physics · doi:10.1007/jhep02(2025)007 · Cited by 14
“…boundary CFT is proportional to the area of a minimal spacelike surface (referred to as the RT surface) that ends on the boundary of 𝐴 in the bulk AdS space 11 , we may See [113] for the covariant generalization. gain new insights into how the gauge structure influences entanglement properties…”
Exploring the bulk in AdS/CFT : A covariant approach
Engelhardt, N. (2017) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.95.066005 · Cited by 14
“the entanglement entropy of progressively larger boundary intervals is understood to probe deeper in the bulk via the Ryu-Takayanagi prescription [17, 18]), in agreement with the expectation that points deep in the bulk are sensitive to dual infrared energy scales.”
BackgroundPhase Transition of AdS Black Holes with Non Linear Source in the Holographic Framework
Moumni, H. E. (2016) · International Journal of Theoretical Physics · doi:10.1007/s10773-016-3197-2 · Cited by 14
Lee, S.-S. (2018) · Journal of High Energy Physics · doi:10.1007/jhep10(2018)043 · Cited by 14
Subregion complexity in holographic thermalization with dS boundary
Zhang, S.-J. (2019) · The European Physical Journal C · doi:10.1140/epjc/s10052-019-7241-2 · Cited by 13
Distinguishing Black Hole Microstates using Holevo Information
Guo, W.-Z., Lin, F.-L., & Zhang, J. (2018) · Physical Review Letters · doi:10.1103/physrevlett.121.251603 · Cited by 14
The holographic dual of the entanglement wedge symplectic form
Kirklin, J. (2020) · Journal of High Energy Physics · doi:10.1007/jhep01(2020)071 · Cited by 15
“In recent years a coherent picture of a particular section of the dictionary, under the heading ‘subregion duality’, has emerged [3–14].”
BackgroundEntwinement as a possible alternative to complexity
Johanna Erdmenger, B., & Gerbershagen, M. (2020) · Journal of High Energy Physics · doi:10.1007/jhep03(2020)082 · Cited by 14
“A further direction worth exploring is a possible generalization of entwinement to find a dual for geodesics not affixed to a constant time slice, in the spirit of the HRT proposal [65] (see also [66] for the related concept of residual entropy).”
BackgroundA model of quantum gravity with emergent spacetime
Lee, S.-S. (2020) · Journal of High Energy Physics · doi:10.1007/jhep06(2020)070 · Cited by 14
Perturbative expansions of Rényi relative divergences and holography
Ugajin, T. (2020) · Journal of High Energy Physics · doi:10.1007/jhep06(2020)053 · Cited by 14
“This idea is supported by the Ryu Takayanagi formula [1, 2] and its covariant generalization [3], which relate the area of particular extremal surfaces in the bulk, to the entanglement entropies in the dual conformal field theory (CFT).”
MethodHolographic entanglement entropy of local quenches in AdS4/CFT3: a finite-element approach
Jahn, A., & Takayanagi, T. (2017) · Refubium (Universitätsbibliothek der Freien Universität Berlin) · doi:10.17169/refubium-2375 · Cited by 14
Self-citationThe evolutions of the innermost stable circular orbits in dynamical spacetimes
Song, Y. (2021) · The European Physical Journal C · doi:10.1140/epjc/s10052-021-09623-6 · Cited by 14
Page curve from dynamical branes in JT gravity
Okuyama, K., & Sakai, K. (2022) · Journal of High Energy Physics · doi:10.1007/jhep02(2022)087 · Cited by 14
Fast scrambling due to rotating shockwaves in BTZ
Malvimat, V., & Poojary, R. R. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.105.126019 · Cited by 14
“puting relevant Ryu-Takayanagi [28, 29] or the covariantized HRT surfaces [30] [8–10].”
BackgroundHolographic coarse-graining: correlators from the entanglement wedge and other reduced geometries
Güijosa, A., Olivas, Y. D., & Pedraza, J. F. (2022) · Journal of High Energy Physics · doi:10.1007/jhep08(2022)118 · Cited by 14
Islands and light gravitons in type IIB string theory
Demulder, S., Gnecchi, A., Lavdas, I., & Lüst, D. (2023) · Journal of High Energy Physics · doi:10.1007/jhep02(2023)016 · Cited by 14
“Advances in this direction rely on a deeper understanding of the calculation of the entropy of Hawking radiation, which has been possible thanks to the identification of a new contribution to the entanglement entropy, following from a quantum generalization [7] of the holographic entanglement entropy prescription [8,…”
BackgroundInfluentialОб островах в черных дырах Шварцшильда
Aref’eva, I. Y., & Volovich, I. V. (2023) · Теоретическая и математическая физика · doi:10.4213/tmf10386 · Cited by 14
Time-evolution of the holographic entanglement entropy and metric perturbationst
Kim, N., & Lee, J. H. (2016) · Journal of the Korean Physical Society · doi:10.3938/jkps.69.623 · Cited by 14
“The Ryu-Takayanagi proposal has been generalized to covariant formulae to suit generic backgrounds in [7], and in this paper we will study the behavior of extremal codimension-two surfaces in backgrounds which are small deformations of pure AdS spacetime.”
MethodFirst law of entanglement rates from holography
O’Bannon, A., Probst, J., Rodgers, R., & Uhlemann, C. F. (2017) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.96.066028 · Cited by 14
“Extremizing A then gives SEE [17, 19], SEE = A[Wext] 4GN .”
BackgroundWhat’s the point? Hole-ography in Poincaré AdS
Espíndola, R., Güijosa, A., Landetta, A., & Pedraza, J. F. (2018) · The European Physical Journal C · doi:10.1140/epjc/s10052-018-5563-0 · Cited by 13
“Their proposal, originally conjectural and referring only to static situations, was extended to the covariant setting in [5] by taking to be an extremal surface, and later proved in”
BackgroundEntropic c–functions in TT‾,JT‾,TJ‾ deformations
Asrat, M. (2020) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2020.115186 · Cited by 17
“We also left out the case F ≥ 0 and μ+ 6= μ− which requires using the Hubeny, Rangamani, and Takayanagi prescription [35].”
MethodInequalities of holographic entanglement of purification from bit threads
Du, D.-H., Shu, F.-W., & Zhu, K.-X. (2020) · The European Physical Journal C · doi:10.1140/epjc/s10052-020-8283-1 · Cited by 14
State-dependent divergences in the entanglement entropy
Marolf, D. M., & Wall, A. C. (2016) · eScholarship (California Digital Library) · Cited by 14
Non-equilibrium steady state formation in 3+1 dimensions
Ecker, C., Johanna Erdmenger, B., & van der Schee, W. (2021) · SciPost Physics · doi:10.21468/scipostphys.11.3.047 · Cited by 14
Gravity from entanglement for boundary subregions
Blanco, D., Leston, M., & Pérez-Nadal, G. (2018) · Journal of High Energy Physics · doi:10.1007/jhep06(2018)130 · Cited by 12
“The RT proposal [2], in its generalized form due to [3], asserts that, for theories with an Einstein gravity dual, the entanglement entropy is obtained by a simple geometric calculation,”
MethodHolographic Entanglement Entropy: A Topical Review*
Chen, B. (2019) · Communications in Theoretical Physics · doi:10.1088/0253-6102/71/7/837 · Cited by 13
Entanglement and chaos in warped conformal field theories
Apolo, L., He, S., Song, W., Xu, J., & Zheng, J. (2019) · MPG.PuRe (Max Planck Society) · Cited by 13
The spacetime geometry of fixed-area states in gravitational systems
Dong, X., Marolf, D. M., Rath, P., Tajdini, A., & Wang, Z. (2022) · Journal of High Energy Physics · doi:10.1007/jhep08(2022)158 · Cited by 13
“Left: starting from a TFD state with inverse temperature β0, fixing the area of the HRT surface γR, corresponding to the time slice τ = 0, results in a Euclidean saddle with a conical singularity (red) with opening angle 2πm, where m = β0β .”
MethodInfluentialAlgebra of operators in an AdS-Rindler wedge
Bahiru, E. (2023) · Journal of High Energy Physics · doi:10.1007/jhep06(2023)197 · Cited by 13
“This will also provide a new renormalization scheme for the area Ryu-Takayanagi surface of a spherical ball subregion of boundary CFTd in d ≥ 2.”
ResultInfluentialHolographic measurement in CFT thermofield doubles
Antonini, S., Grado-White, B., Jian, S.-K., & Swingle, B. G. (2023) · Journal of High Energy Physics · doi:10.1007/jhep07(2023)014 · Cited by 13
A modified cosmic brane proposal for holographic Renyi entropy
Dong, X., Kudler-Flam, J., & Rath, P. (2024) · Journal of High Energy Physics · doi:10.1007/jhep06(2024)120 · Cited by 16
Off-shell strings II: Black hole entropy
Ahmadain, A. A., & Wall, A. C. (2024) · SciPost Physics · doi:10.21468/scipostphys.17.1.006 · Cited by 28
Kudler-Flam, J., Masahiro Nozaki, A., Numasawa, T., Ryu, S., & Tan, M. T. (2024) · Journal of High Energy Physics · doi:10.1007/jhep08(2024)213 · Cited by 13
“Through the holographic entanglement entropy formula [65–67], the entanglement entropy measures the distance between AdS boundary and the EOW brane.”
Caputa, P., Chen, B., Takayanagi, T., & Tsuda, T. (2025) · Journal of High Energy Physics · doi:10.1007/jhep01(2025)003 · Cited by 13
Self-citationTimelike entanglement entropy: A top-down approach
Núñez, C., & Dibakar Roychowdhury, B. (2025) · Physical review. D/Physical review. D. · doi:10.1103/vjyt-xc15 · Cited by 13
Localized excitations from localized unitary operators
Sivaramakrishnan, A. (2017) · Annals of Physics · doi:10.1016/j.aop.2017.03.012 · Cited by 12
“This investigation may be useful in the AdS/CFT correspondence through the Hubeny-Rangamani-Takayanagi conjecture, and as part of the entanglement tsunami picture [34–37].”
MethodHolographic entanglement entropy of local quenches in AdS4/CFT3: a finite-element approach
Jahn, A., & Takayanagi, T. (2017) · Journal of Physics A Mathematical and Theoretical · doi:10.1088/1751-8121/aa8afa · Cited by 13
“In particular, AdS/CFT provides a geometrical method to compute entanglement entropy [3, 4] (see [5, 6] for its derivations).”
MethodSelf-citationSaturation of the quantum null energy condition in far-from-equilibrium systems
Ecker, C., Grumiller, D., van der Schee, W., & Stanzer, P. (2018) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.97.126016 · Cited by 13
Bulk matter and the boundary quantum null energy condition
Khandker, Z. U., Kundu, S., & Li, D. (2018) · Journal of High Energy Physics · doi:10.1007/jhep08(2018)162 · Cited by 13
Lectures on bulk reconstruction
Kajuri, N. (2021) · SciPost Physics Lecture Notes · doi:10.21468/scipostphyslectnotes.22 · Cited by 31
“e region we rst recall the covariant version of the Ryu-Takayangi proposal (usually called the HRT or Hubeny-Rangamani-Takayanagi proposal) for holographic entanglement entropy of a boundary region R [38,39]. According to the HRT proposal, the entanglement entropy of R is equal to the area of the extremal surface R, w…”
The holographic dual of the entanglement wedge symplectic form
Kirklin, J. (2019) · Apollo (University of Cambridge) · doi:10.17863/cam.53403 · Cited by 13
Jiang, Y., Kim, M., & Wong, G. (2021) · Journal of High Energy Physics · doi:10.1007/jhep10(2021)202 · Cited by 16
Erasure Tolerant Quantum Memory and the Quantum Null Energy Condition in Holographic Systems
Banerjee, A., Kibe, T., Mittal, N., Mukhopadhyay, A., & Roy, P. (2022) · Physical Review Letters · doi:10.1103/physrevlett.129.191601 · Cited by 13
Ðorđević, S., Gočanin, A., Gočanin, D., & Radovanović, V. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.105015 · Cited by 13
Lin, Y.-Y. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.106010 · Cited by 13
Geometrizing the partial entanglement entropy: from PEE threads to bit threads
Lin, J., Lu, Y., & Wen, Q. (2024) · Journal of High Energy Physics · doi:10.1007/jhep02(2024)191 · Cited by 13
“In the context of AdS / CFT correspondence [ 1 ] , the Ryu-Takayanagi (RT) formula [ 2–4 ] un-covers a relation between bulk geometry and boundary entanglement, by claiming that the entanglement entropy (EE) S A for a region A in the boundary CFT is given by the area of a minimal surface E A…”
MethodGravity from entanglement and RG flow in a top-down approach
Kwon, O.-K., Jang, D., Kim, Y., & Tolla, D. D. (2018) · Journal of High Energy Physics · doi:10.1007/jhep05(2018)009 · Cited by 13
“The holographic calculation of the EE, which was proposed by Ryu and Takayanagi (RT) [1, 2] and its covariant generalization [3], drew much attention due to its elegance and implications in condensed matter physics and gravity theories.”
MethodA note on islands in Schwarzschild black holes
Aref’eva, I. Y., & Volovich, I. V. (2023) · Theoretical and Mathematical Physics · doi:10.1134/s004057792303008x · Cited by 12
“Although the prescription of the extremal quantum surface was proposed in the framework of holography [23], [24], the island rule is applicable to black holes in more general theories.”
BackgroundExactly stable collective oscillations in conformal field theory
Freivogel, B., McGreevy, J., & Suh, S. J. (2012) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.85.105002 · Cited by 13
Double‐trace deformations and entanglement entropy in AdS
Miyagawa, T., Shiba, N., & Takayanagi, T. (2016) · Fortschritte der Physik · doi:10.1002/prop.201500098 · Cited by 13
“One such example is the holographic calculation of entanglement entropy [4].”
BackgroundSelf-citationSchwarzschild de Sitter and extremal surfaces
Fernandes, K., Kolekar, K. S., Narayan, K., & Roy, S. (2020) · The European Physical Journal C · doi:10.1140/epjc/s10052-020-08437-2 · Cited by 14
“inates and Penrose diagrams 17 B SdS3 and extremal surfaces 18 C Analytic expressions for the area integrals 20 1 Introductionand summary Over the last several years, holographic entanglement entropy [1, 2, 3, 4] has been under substantial investigation, both from the point of view of gaining new insights on strongly…”
BackgroundAbsolute entropy and the observer’s no-boundary state
Blommaert, A., Kudler-Flam, J., & Urbach, E. Y. (2025) · Journal of High Energy Physics · doi:10.1007/jhep11(2025)113 · Cited by 33
First law of entanglement entropy in flat-space holography
Fareghbal, R., & Shalamzari, M. H. (2019) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.100.106006 · Cited by 12
“Recently, a prescription (similar to the Ryu-Takayanagi’s proposal for the CFT entanglement entropy [16, 17]) has been proposed for the BMSFT entanglememnt entropy [12] that relates it to the area of some particular”
MethodGlobal aspects of conformal symmetry and the ANEC in dS and AdS
Rosso, F. (2020) · Journal of High Energy Physics · doi:10.1007/jhep03(2020)186 · Cited by 12
“J H E P 0 3 ( 2 0 2 0 ) 1 8 6 two independent approaches; the first one based on some symmetry considerations and the second on the HRRT holographic prescription [33, 34].”
BackgroundA tale of two butterflies: an exact equivalence in higher-derivative gravity
Dong, X., Wang, D., Weng, W. W., & Wu, C.-H. (2022) · Journal of High Energy Physics · doi:10.1007/jhep10(2022)009 · Cited by 12
“Note that even though the location of the particle is time-dependent, the background spacetime is static6 and at any given time we may use a Ryu-Takayanagi (RT) surface [26, 27] (instead of its dynamical generalization — the HRT surface [28]).”
Islands in the fluid: islands are common in cosmology
Ben-Dayan, I., Hadad, M., & Wildenhain, E. (2023) · Journal of High Energy Physics · doi:10.1007/jhep03(2023)077 · Cited by 12
Statistical mechanics of monitored dissipative random circuits
Li, Y., & Claassen, M. (2023) · Physical review. B./Physical review. B · doi:10.1103/physrevb.108.104310 · Cited by 12
Entanglement entropy for spherically symmetric regular black holes
Luongo, O., Mancini, S., & Pierosara, P. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.104059 · Cited by 12
Pseudo entropy under joining local quenches
Shinmyo, K., Takayanagi, T., & Tasuki, K. (2024) · Journal of High Energy Physics · doi:10.1007/jhep02(2024)111 · Cited by 12
Self-citationIsland of Reissner-Nordström anti–de Sitter black holes in the large D limit
Tong, C.-W., Du, D.-H., & Sun, J.-R. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.109.104053 · Cited by 12
“This formula comes from the holographic entanglement entropy(HEE) formula (or RT formula) [10, 11] and its quantum version, i.e. the quantum extremal surface (QES) [12, 13].”
BackgroundBlack hole singularity and timelike entanglement
Anegawa, T., & Tamaoka, K. (2024) · Journal of High Energy Physics · doi:10.1007/jhep10(2024)182 · Cited by 12
“The entanglement entropy, the unique measure of bi-partite entanglement for pure states, can capture the spatial structure of spacetime through the spacelike extremal surfaces in the bulk [3, 6].”
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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