REVIEW 2 major objections 5 minor 1 cited by
Open Virasoro TQFT computes open-sector 3d gravity path integrals with fixed lengths above threshold and fixed angles below, and open-closed duality explains the CTV–scalar Virasoro relation.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · grok-4.5
2026-07-14 19:46 UTC pith:P62JI5YF
load-bearing objection Solid open-sector extension that re-derives the CTV–Virasoro identity via open-closed duality; the gravity dictionary is proposed by analogy and remains the soft spot. the 2 major comments →
The many facets of a hyperbolic tetrahedron: open and closed triangulations of 3d gravity
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The open Virasoro TQFT partition function equals the gravitational path integral on a compact region with fixed-length boundary conditions for above-threshold open states and fixed-angle (kink) boundary conditions for below-threshold open states. For the special subclass of manifolds built only from boundary Wilson loops, the same partition function, after an open-closed duality implemented by modular S-transforms, is identical to the Conformal Turaev-Viro partition function and therefore to the absolute square of a scalar closed Virasoro TQFT partition function.
What carries the argument
Open Virasoro TQFT, whose building block is the open 6j manifold (a truncated tetrahedron with four EOW faces and four OPE faces). Gluing these 6j symbols along disks and performing annular surgery on closed Wilson loops is dual to tetrahedral decomposition of the compact manifold; the open-closed duality (annulus modular S-transform) then converts kink loops into bulk scalar Wilson lines.
Load-bearing premise
The central dictionary that equates the fixed-length gravitational path integral to the open Virasoro TQFT partition function is proposed by direct analogy with the closed-sector result rather than derived from a first-principles variational principle for the open action.
What would settle it
Compute the classical volume of a simple open saddle (for example the single truncated tetrahedron or the four-tetrahedron gluing with all external lengths equal) both from the Einstein-Hilbert-plus-Hayward action and from the semiclassical limit of the corresponding open 6j symbol; any systematic mismatch falsifies the claimed equality.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper isolates a purely open sector of 3d gravity dual to open BCFT data (boundary spectra, boundary OPE coefficients, and g-functions), formulated as open Virasoro TQFT obtained by restricting the open-closed theory to admissible manifolds with EOW branes. It proposes that this TQFT computes gravitational path integrals on compact regions whose boundaries consist of EOW branes and pleated surfaces, with fixed-length conditions for above-threshold states and fixed-angle (kink) conditions for below-threshold states. Manifolds are constructed by gluing truncated tetrahedra (equivalently, open 6j manifolds plus annular surgery). For the special subclass involving only boundary Wilson loops, an open-closed duality via the modular S-kernel is used to re-derive the relation between Conformal Turaev-Viro theory and the scalar sector of two copies of Virasoro TQFT.
Significance. The isolation of a purely open ensemble is useful: it removes modular constraints on the spectral density and reduces the set of contributing manifolds, while still capturing nontrivial OPE statistics and wormhole geometries. The triangulation technology (truncated tetrahedra with EOW/OPE faces, Gram-matrix length/angle data, annular surgery dual to internal edges) is concrete and illustrated with an explicit four-tetrahedron volume computation. The open-closed duality derivation of the CTV–scalar Virasoro relation is a clean conceptual contribution that avoids chain-mail invariants and clarifies why CTV computes fixed-angle ensembles. These results strengthen the dictionary between Virasoro TQFT, BCFT ensembles, and hyperbolic 3-manifolds with branes.
major comments (2)
- [§2.3–2.4, eqs. (2.39), (2.49)] §2.3–2.4, eqs. (2.39) and (2.49): The central gravity dictionary Z_L[M,γ(P)] = ˆZ_oVir[M_E,Γ(P)] is introduced solely by analogy with Hartman’s closed-sector result. After defining the open actions I_L and I_A (including Hayward terms), the text states “By analogy with the closed case [39], we propose…” and then “therefore identify.” The only explicit check is the zero-volume Θ-graph saddle recovering |B̂|^2 ⊃ 1. No independent saddle-point evaluation of I_L (or I_A) is given for a positive-volume manifold with internal edges (e.g. the four-tetrahedron gluing of §3.1 whose volume is computed numerically as 9.276). Because the abstract and introduction present this identification as established (“We show that it computes…”), the claim needs either a first-principles variational argument for the open Neumann/EOW setting, a non-trivial semiclassical match, or a clear reframing as a proposal
- [§4.2, eq. (4.6)] §4.2, eq. (4.6): The reduction of CTV to open Virasoro TQFT when all OPE faces are glued is asserted by reading the fixed-angle path integral identically to (3.20) with tensionless branes and imaginary weights. While the subsequent modular-S steps (4.8)–(4.12) are standard and cleanly presented, the identification itself inherits the same dictionary status as (2.49). If the open gravity dictionary is only analogical, the geometric interpretation of CTV as a fixed-angle ensemble remains conditional even though the purely algebraic map between open TQFT and |ˆZ_Vir|^2 is intact. A short clarification of which statements are algebraic identities versus geometric interpretations would protect the CTV result.
minor comments (5)
- [Abstract, §1] Abstract and Introduction: Replace “We show that it computes gravitational path integrals…” with language matching the body (“we propose / identify by analogy”), so that the abstract does not overstate the status of (2.49).
- [§3.1] §3.1: The numerical example (external lengths 1.000 → ℓ_M = 4.086, volume 9.276) is welcome; stating the classical 6j asymptotics used for the volume formula and, if feasible, comparing to the leading log of the corresponding open TQFT integral would strengthen the semiclassical link.
- [§2.4] Notation: The hat on ˆZ_oVir / ˆB is introduced as a normalization choice that also turns junctions into Neumann disks; a single sentence early in §2.4 collecting both meanings would help readers who jump between sections.
- [Fig. 2, Table 1] Figure 2 caption and Table 1: Both are useful; ensure the printed version keeps the color coding (green EOW / orange corners / red kinks) distinguishable in grayscale, or add hatch patterns.
- [§2.4] Typos: “therefor identify” → “therefore identify” (after (2.48)); “igcup” style products in the skeptic note are not in the PDF but check for similar OCR/typesetting artifacts in the arXiv source if any remain.
Circularity Check
Central open gravity–TQFT dictionary (Z_L = hat Z_oVir) is proposed by analogy to Hartman rather than derived, so fixed-length/angle claims rest on that identification; CTV rederivation itself is non-circular.
specific steps
-
other
[§2.3–2.4, eqs. (2.39) and (2.49)]
"By analogy with the closed case [39], we propose that igcup_e (g_a g_b)^{1/2} igcup_v B̂^{(abc)}_{IJK} = igcup_M Z_L[M, au(P)]. o From (2.39), we therefore identify Z_L[M, au(P)] = hat Z_oVir[M_E, au(P)]."
The equality that lets the paper claim “open Virasoro TQFT computes gravitational path integrals with fixed-length/angle BCs” is not derived from the open Einstein–Hilbert + Hayward + EOW action; it is postulated by direct analogy to Hartman’s closed-sector result. Once postulated, every later statement that a given open TQFT diagram equals a gravity path integral follows by definition of the identification. The only check offered is the trivial zero-volume heta-graph already known from BCFT bootstrap; no independent saddle is computed for any manifold with internal edges or positive volume. Thus the strongest claim reduces to the proposal itself.
-
self citation load bearing
[§2.4 and §3.2 (definition of open Virasoro TQFT and annular surgery)]
"The open Virasoro TQFT can then be built from the remaining condition, namely the crossing symmetry of four boundary operators on the disk [35]. o gluing open 6j manifolds and performing annular surgeries is the same as a tetrahedral decomposition"
The ambient open Virasoro TQFT (6j symbols, annular surgery, normalization of junctions) is taken wholesale from the authors’ own prior work [35]. While normal for a follow-up paper, the geometric interpretation of those same diagrams as gravity path integrals with the new fixed-length/angle dictionary inherits the earlier construction without re-deriving the open TQFT axioms or the surgery rules from the open gravitational action. The load is therefore partially self-referential, though secondary to the analogy step above.
full rationale
The paper’s strongest claim—that open Virasoro TQFT computes gravitational path integrals on compact regions with fixed-length (above-threshold) and fixed-angle (below-threshold) boundary conditions—is introduced in §2.3–2.4 solely by the sentence “By analogy with the closed case [39], we propose that igcup(g_a g_b)^{1/2} igcup B̂ = igcup_M Z_L o therefore identify Z_L = hat Z_oVir.” No independent saddle-point evaluation of the open action I_L/I_A (Hayward terms + EOW Neumann) is performed for any positive-volume manifold, nor is a first-principles variational derivation supplied. The only explicit check is the zero-volume heta-graph that recovers the already-known |B̂|^2 i 1. Once the identification is assumed, every subsequent geometric interpretation of open TQFT diagrams as gravity path integrals follows by construction. This is mild circularity of the “proposed dictionary = claimed result” type, not a fitted-parameter or uniqueness-theorem loop. By contrast, the rederivation of the CTV–scalar-Virasoro relation (1.1)/(4.1) is independent: it equates CTV (by its triangulation definition) to the special case of open TQFT with only Wilson loops, then applies the standard modular S-kernel (open-closed duality) and obtains the known Fourier relation; that algebraic step does not rely on the gravity dictionary and is not circular. Self-citations to the authors’ prior open-closed TQFT construction [35] are present but load-bearing only for the ambient formalism, not for the new claims. No parameters are fitted to data and then re-predicted; no uniqueness theorem is imported from the authors’ own prior work. Overall score 3 reflects one load-bearing analogy that makes the gravity claim definitional on its own proposal, while the purely algebraic CTV argument remains self-contained.
Axiom & Free-Parameter Ledger
axioms (5)
- domain assumption AdS/BCFT dictionary equating BCFT partition functions on bordered surfaces to sums over hyperbolic 3-manifolds with EOW branes (eq. 2.1)
- domain assumption Open-closed Virasoro TQFT exists and satisfies the six Moore-Seiberg conditions of BCFT; the purely open sector is obtained by retaining only the four-boundary-operator crossing relation
- domain assumption Only manifolds that admit hyperbolic saddles under the Einstein-Hilbert + EOW action contribute; non-hyperbolic contributions are discarded
- ad hoc to paper The closed-sector fixed-length dictionary of Hartman [39] continues to hold after open restriction, so Z_L = hat Z_oVir (eq. 2.49)
- standard math Modular S-kernel on the annulus implements open-closed duality for scalar states (eq. 4.8)
invented entities (2)
-
open Virasoro TQFT (restriction of open-closed Virasoro TQFT to admissible open manifolds)
no independent evidence
-
open truncated tetrahedra / open 6j manifolds with EOW faces and OPE faces
no independent evidence
read the original abstract
We study a model of 3d gravity relevant to the open sector of a CFT ensemble. The quantum theory is the open Virasoro TQFT, obtained by restricting the full open-closed Virasoro TQFT to a subclass of admissible manifolds. We show that it computes gravitational path integrals on compact regions with fixed-length boundary conditions for states above the black hole threshold, and fixed-angle boundary conditions for states below the threshold. Focusing on a special class of manifolds involving only boundary Wilson loops, we further show that the relation between Conformal Turaev-Viro theory and the diagonal sector of two copies of Virasoro TQFT arises naturally from an open-closed duality.
Forward citations
Cited by 1 Pith paper
-
A Holographic Map from AdS$_3$ to CFT$_2$
Semiclassical pure AdS3 gravity states, labelled by fixed-area geodesic networks, are mapped to CFT2 primary states whose wavefunctions are networks of OPE coefficients.
Reference graph
Works this paper leans on
-
[1]
Achucarro and P
A. Achucarro and P. K. Townsend,A Chern-Simons Action for Three-Dimensional anti-De Sitter Supergravity Theories,Phys. Lett. B180(1986) 89
1986
-
[2]
Witten,(2+1)-Dimensional Gravity as an Exactly Soluble System,Nucl
E. Witten,(2+1)-Dimensional Gravity as an Exactly Soluble System,Nucl. Phys. B 311(1988) 46
1988
-
[3]
P. Kraus and A. Maloney,A cardy formula for three-point coefficients or how the black hole got its spots,JHEP05(2017) 160 [1608.03284]
Pith/arXiv arXiv 2017
-
[4]
J. Cardy, A. Maloney and H. Maxfield,A new handle on three-point coefficients: OPE asymptotics from genus two modular invariance,JHEP10(2017) 136 [1705.05855]
Pith/arXiv arXiv 2017
-
[5]
S. Collier, A. Maloney, H. Maxfield and I. Tsiares,Universal dynamics of heavy operators in CFT 2,JHEP07(2020) 074 [1912.00222]
Pith/arXiv arXiv 2020
-
[6]
A. Belin and J. de Boer,Random statistics of OPE coefficients and Euclidean wormholes,Class. Quant. Grav.38(2021) 164001 [2006.05499]
Pith/arXiv arXiv 2021
-
[7]
A. Belin, J. de Boer and D. Liska,Non-Gaussianities in the statistical distribution of heavy OPE coefficients and wormholes,JHEP06(2022) 116 [2110.14649]
Pith/arXiv arXiv 2022
-
[8]
T. Anous, A. Belin, J. de Boer and D. Liska,OPE statistics from higher-point crossing, JHEP06(2022) 102 [2112.09143]
Pith/arXiv arXiv 2022
-
[9]
J. Chandra, S. Collier, T. Hartman and A. Maloney,Semiclassical 3D gravity as an average of large-c CFTs,JHEP12(2022) 069 [2203.06511]
Pith/arXiv arXiv 2022
-
[10]
S. Collier, L. Eberhardt and M. Zhang,Solving 3d gravity with Virasoro TQFT, SciPost Phys.15(2023) 151 [2304.13650]
Pith/arXiv arXiv 2023
-
[11]
A. Belin, J. de Boer, D. L. Jafferis, P. Nayak and J. Sonner,Approximate CFTs and random tensor models,JHEP09(2024) 163 [2308.03829]
Pith/arXiv arXiv 2024
-
[12]
J. de Boer, D. Liska, B. Post and M. Sasieta,A principle of maximum ignorance for semiclassical gravity,JHEP2024(2024) 003 [2311.08132]
Pith/arXiv arXiv 2024
-
[13]
S. Collier, L. Eberhardt and M. Zhang,3d gravity from Virasoro TQFT: Holography, wormholes and knots,SciPost Phys.17(2024) 134 [2401.13900]. – 30 –
Pith/arXiv arXiv 2024
-
[14]
J. de Boer, D. Liska and B. Post,Multiboundary wormholes and OPE statistics,JHEP 10(2024) 207 [2405.13111]
Pith/arXiv arXiv 2024
-
[15]
D. L. Jafferis, L. Rozenberg and G. Wong,3d gravity as a random ensemble,JHEP02 (2025) 208 [2407.02649]
Pith/arXiv arXiv 2025
-
[16]
Chandra,Statistics in 3d gravity from knots and links,JHEP12(2025) 139 [2508.10864]
J. Chandra,Statistics in 3d gravity from knots and links,JHEP12(2025) 139 [2508.10864]
Pith/arXiv arXiv 2025
- [17]
-
[18]
Wang,Crossing symmetry of OPE statistics,2512.21258
D. Wang,Crossing symmetry of OPE statistics,2512.21258
-
[19]
A. Maloney and E. Witten,Quantum Gravity Partition Functions in Three Dimensions,JHEP02(2010) 029 [0712.0155]
Pith/arXiv arXiv 2010
-
[20]
C. A. Keller and A. Maloney,Poincare Series, 3D Gravity and CFT Spectroscopy, JHEP02(2015) 080 [1407.6008]
Pith/arXiv arXiv 2015
-
[21]
J. Cotler and K. Jensen,AdS 3 gravity and random CFT,JHEP04(2021) 033 [2006.08648]
Pith/arXiv arXiv 2021
-
[22]
H. Maxfield and G. J. Turiaci,The path integral of 3D gravity near extremality; or, JT gravity with defects as a matrix integral,JHEP01(2021) 118 [2006.11317]
Pith/arXiv arXiv 2021
-
[23]
G. Di Ubaldo and E. Perlmutter,AdS 3/RMT2 duality,JHEP12(2023) 179 [2307.03707]
Pith/arXiv arXiv 2023
- [24]
-
[25]
Witten,Quantum Field Theory and the Jones Polynomial,Commun
E. Witten,Quantum Field Theory and the Jones Polynomial,Commun. Math. Phys. 121(1989) 351
1989
-
[26]
Takayanagi,Holographic Dual of BCFT,Phys
T. Takayanagi,Holographic Dual of BCFT,Phys. Rev. Lett.107(2011) 101602 [1105.5165]
Pith/arXiv arXiv 2011
-
[27]
M. Fujita, T. Takayanagi and E. Tonni,Aspects of AdS/BCFT,JHEP11(2011) 043 [1108.5152]
Pith/arXiv arXiv 2011
-
[28]
D. Wang, Z. Wang and Z. Wei,Wormholes with ends of the world,JHEP09(2025) 166 [2504.12278]
arXiv 2025
-
[29]
Y. Kusuki,Analytic bootstrap in 2D boundary conformal field theory: towards braneworld holography,JHEP03(2022) 161 [2112.10984]
Pith/arXiv arXiv 2022
-
[30]
T. Numasawa and I. Tsiares,Universal dynamics of heavy operators in boundary CFT2,JHEP08(2022) 156 [2202.01633]
Pith/arXiv arXiv 2022
-
[31]
H. Geng,Aspects of AdS 2 quantum gravity and the Karch-Randall braneworld,JHEP 09(2022) 024 [2206.11277]. – 31 –
Pith/arXiv arXiv 2022
-
[32]
C. I. Lazaroiu,On the structure of open - closed topological field theory in two-dimensions,Nucl. Phys. B603(2001) 497 [hep-th/0010269]
Pith/arXiv arXiv 2001
-
[33]
A. D. Lauda and H. Pfeiffer,Open-closed strings: Two-dimensional extended TQFTs and Frobenius algebras,math/0510664
-
[34]
G. W. Moore and G. Segal,D-branes and K-theory in 2D topological field theory, hep-th/0609042
-
[35]
D. L. Jafferis, L. Rozenberg and D. Wang,Open-closed 3d gravity as a random ensemble,JHEP10(2025) 228 [2506.19817]
arXiv 2025
-
[36]
S. Collier, L. Eberhardt, B. M¨ uhlmann and V. A. Rodriguez,The Virasoro minimal string,SciPost Phys.16(2024) 057 [2309.10846]
Pith/arXiv arXiv 2024
-
[37]
D. L. Jafferis, L. Rozenberg, D. Sarkar and D. Wang,On random matrix statistics of 3d gravity,2512.05045
-
[38]
L.-Y. Hung, Y. Jiang and B.-X. Lao,Universal Structures and Emergent Geometry from Large-cBCFT Ensemble,2504.21660
-
[39]
Hartman,Triangulating quantum gravity in AdS 3,2507.12696
T. Hartman,Triangulating quantum gravity in AdS 3,2507.12696
-
[40]
J. W. Barrett, J. M. Garcia-Islas and J. F. Martins,Observables in the Turaev-Viro and Crane-Yetter models,J. Math. Phys.48(2007) 093508 [math/0411281]
Pith/arXiv arXiv 2007
-
[41]
F. J. Burnell and S. H. Simon,Space-Time Geometry of Topological phases,Annals Phys.325(2010) 2550 [1004.5586]
Pith/arXiv arXiv 2010
-
[42]
V. G. Turaev and O. Y. Viro,State sum invariants of 3-manifolds and quantum 6 j-symbols,Topology31(1992) 865
1992
-
[43]
Hartman,Conformal Turaev-Viro Theory,2507.11652
T. Hartman,Conformal Turaev-Viro Theory,2507.11652
-
[44]
J. M. Maldacena and L. Maoz,Wormholes in AdS,JHEP02(2004) 053 [hep-th/0401024]
Pith/arXiv arXiv 2004
-
[45]
J.-M. Schlenker and E. Witten,No ensemble averaging below the black hole threshold, JHEP07(2022) 143 [2202.01372]
Pith/arXiv arXiv 2022
-
[46]
A. Karch and L. Randall,Locally localized gravity,JHEP05(2001) 008 [hep-th/0011156]
Pith/arXiv arXiv 2001
-
[47]
A. Karch and L. Randall,Open and closed string interpretation of SUSY CFT’s on branes with boundaries,JHEP06(2001) 063 [hep-th/0105132]
Pith/arXiv arXiv 2001
-
[48]
D. Marolf and H. Maxfield,Transcending the ensemble: baby universes, spacetime wormholes, and the order and disorder of black hole information,JHEP08(2020) 044 [2002.08950]
Pith/arXiv arXiv 2020
-
[49]
J. L. Cardy,Conformal Invariance and Surface Critical Behavior,Nucl. Phys. B240 (1984) 514. – 32 –
1984
-
[50]
H. L. Verlinde,Conformal Field Theory, 2-DQuantum Gravity and Quantization of Teichmuller Space,Nucl. Phys. B337(1990) 652
1990
-
[51]
H. Dorn and H. J. Otto,Two and three point functions in Liouville theory,Nucl. Phys. B429(1994) 375 [hep-th/9403141]
Pith/arXiv arXiv 1994
-
[52]
A. B. Zamolodchikov and A. B. Zamolodchikov,Structure constants and conformal bootstrap in Liouville field theory,Nucl. Phys. B477(1996) 577 [hep-th/9506136]
Pith/arXiv arXiv 1996
-
[53]
M. Miyaji and C. Murdia,Holographic BCFT with a Defect on the End-of-the-World brane,JHEP11(2022) 123 [2208.13783]
Pith/arXiv arXiv 2022
-
[54]
Hayward,Gravitational action for space-times with nonsmooth boundaries,Phys
G. Hayward,Gravitational action for space-times with nonsmooth boundaries,Phys. Rev. D47(1993) 3275
1993
-
[55]
G. W. Moore and N. Seiberg,Polynomial Equations for Rational Conformal Field Theories,Phys. Lett. B212(1988) 451
1988
-
[56]
G. W. Moore and N. Seiberg,Classical and Quantum Conformal Field Theory, Commun. Math. Phys.123(1989) 177
1989
-
[57]
J. L. Cardy and D. C. Lewellen,Bulk and boundary operators in conformal field theory, Phys. Lett. B259(1991) 274
1991
-
[58]
D. C. Lewellen,Sewing constraints for conformal field theories on surfaces with boundaries,Nucl. Phys. B372(1992) 654
1992
-
[59]
J. Teschner and G. Vartanov,6j symbols for the modular double, quantum hyperbolic geometry, and supersymmetric gauge theories,Lett. Math. Phys.104(2014) 527 [1202.4698]
Pith/arXiv arXiv 2014
-
[60]
J. Teschner and G. S. Vartanov,Supersymmetric gauge theories, quantization ofM flat, and conformal field theory,Adv. Theor. Math. Phys.19(2015) 1 [1302.3778]
Pith/arXiv arXiv 2015
-
[61]
Eberhardt,Notes on crossing transformations of Virasoro conformal blocks, 2309.11540
L. Eberhardt,Notes on crossing transformations of Virasoro conformal blocks, 2309.11540
-
[62]
B. Ponsot and J. Teschner,Liouville bootstrap via harmonic analysis on a noncompact quantum group,hep-th/9911110
-
[63]
B. Ponsot and J. Teschner,Clebsch-Gordan and Racah-Wigner coefficients for a continuous series of representations of U(q)(sl(2,R)),Commun. Math. Phys.224 (2001) 613 [math/0007097]
Pith/arXiv arXiv 2001
-
[64]
W. P. Thurston,Hyperbolic structures on 3-manifolds i: Deformation of acylindrical manifolds,Annals of Mathematics124(1986) 203
1986
-
[65]
Ushijima,A volume formula for generalised hyperbolic tetrahedra, inNon-Euclidean Geometries: J´ anos Bolyai Memorial Volume, pp
A. Ushijima,A volume formula for generalised hyperbolic tetrahedra, inNon-Euclidean Geometries: J´ anos Bolyai Memorial Volume, pp. 249–265. Springer, 2006
2006
-
[66]
Roberts,Skein theory and Turaev-Viro invariants,Topology34(1995)
J. Roberts,Skein theory and Turaev-Viro invariants,Topology34(1995) . – 33 –
1995
-
[67]
J. W. Barrett,Geometrical measurements in three-dimensional quantum gravity,Int. J. Mod. Phys. A18S2(2003) 97 [gr-qc/0203018]
Pith/arXiv arXiv 2003
-
[68]
J. M. Garcia-Islas,Observables in three-dimensional quantum gravity and topological invariants,Class. Quant. Grav.21(2004) 3933 [gr-qc/0401093]
Pith/arXiv arXiv 2004
-
[69]
L. Y. Hung and G. Wong,Entanglement branes and factorization in conformal field theory,Phys. Rev. D104(2021) 026012 [1912.11201]
Pith/arXiv arXiv 2021
-
[70]
E. M. Brehm and I. Runkel,Lattice models from CFT on surfaces with holes: I. Torus partition function via two lattice cells,J. Phys. A55(2022) 235001 [2112.01563]
Pith/arXiv arXiv 2022
-
[71]
L. Chen, K. Ji, H. Zhang, C. Shen, R. Wang, X. Zeng et al.,CFTD from TQFTD+1 via Holographic Tensor Network, and Precision Discretization of CFT2,Phys. Rev. X 14(2024) 041033 [2210.12127]
Pith/arXiv arXiv 2024
-
[72]
G. Cheng, L. Chen, Z.-C. Gu and L.-Y. Hung,Precision Reconstruction of Rational Conformal Field Theory from Exact Fixed-Point Tensor Network,Phys. Rev. X15 (2025) 011073 [2311.18005]
Pith/arXiv arXiv 2025
-
[73]
E. M. Brehm and I. Runkel,Lattice models from CFT on surfaces with holes II: Cloaking boundary conditions and loop models,2410.19938
-
[74]
L. Chen, L.-Y. Hung, Y. Jiang and B.-X. Lao,Deriving the non-perturbative gravitational dual of quantum Liouville theory from BCFT operator algebra,SciPost Phys.19(2025) 163 [2403.03179]
arXiv 2025
-
[75]
L.-Y. Hung and Y. Jiang,Building up quantum spacetimes with BCFT Legos, 2404.00877
-
[76]
N. Bao, L.-Y. Hung, Y. Jiang and Z. Liu,QG from SymQRG: AdS 3/CFT2 Correspondence as Topological Symmetry-Preserving Quantum RG Flow,2412.12045
-
[77]
H. Geng, L.-Y. Hung and Y. Jiang,It from ETH: Multi-interval Entanglement and Replica Wormholes from Large-cBCFT Ensemble,2505.20385. – 34 –
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.