Genuine multientropy, dihedral invariants and Lifshitz theory
Pith reviewed 2026-05-18 19:16 UTC · model grok-4.3
The pith
Genuine multientropy for Lifshitz ground states equals mutual information plus logarithmic negativity and continues analytically to non-integer Rényi indices.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
For Lifshitz ground states the genuine multientropy is computed explicitly via the replica method and continued analytically to non-integer Rényi indices. It reduces to a combination of mutual information and logarithmic negativity, a reduction that also holds for stabilizer states. Dihedral invariants on replica states for any tripartite pure state are equivalent to Rényi reflected entropies because dihedral permutations realize the reflected replica construction or, equivalently, the realignment operation on density matrices.
What carries the argument
Genuine multientropy as a multi-invariant of state replicas, computed through the replica construction in Lifshitz ground states.
If this is right
- The reduction allows multientropy to be evaluated from standard bipartite entanglement measures in Lifshitz systems and stabilizer states.
- Analytic continuation supplies a definition of multientropy for non-integer Rényi indices without further regularization.
- Dihedral invariants supply an alternative replica route to Rényi reflected entropies for any tripartite pure state.
- Replica permutations under the dihedral group are equivalent to the reflected replica construction or to realignment of density matrices.
Where Pith is reading between the lines
- If the reduction extends beyond Lifshitz and stabilizer states it would simplify multipartite entanglement calculations across a broader class of many-body systems.
- Linking multientropy to reflected entropies could unify different replica-based probes of higher-order correlations in quantum field theory.
- The same techniques might be tested on other scale-invariant critical points to extract universal multipartite features.
Load-bearing premise
The replica construction for Lifshitz ground states admits a well-defined analytic continuation in the Rényi index that preserves the quantity as a valid entanglement monotone.
What would settle it
An explicit calculation of genuine multientropy for a concrete Lifshitz ground state at a non-integer Rényi index that fails to match the combination of mutual information and logarithmic negativity would falsify the reduction.
Figures
read the original abstract
Multi-invariants are local-unitary invariants of state replicas introduced as potential probes of multipartite entanglement and correlations in quantum many-body systems. In this paper, we investigate two multi-invariants for tripartite pure states, namely multientropy and dihedral invariant. We compute the (genuine) multientropy for Lifshitz groundstates, and obtain its analytical continuation to noninteger values of R\'enyi index. We show that the genuine multientropy can be expressed in terms of mutual information and logarithmic negativity, a relation that also holds for stabilizer states. For general tripartite pure states, we demonstrate that dihedral invariants are related to R\'enyi reflected entropies. In particular, we show that the dihedral permutations of replicas are equivalent to the reflected construction, or alternatively to the realignment of density matrices.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript investigates multi-invariants for tripartite pure states, focusing on multientropy and the dihedral invariant. It computes the genuine multientropy for Lifshitz ground states and obtains its analytical continuation to non-integer values of the Rényi index. The authors show that the genuine multientropy can be expressed in terms of mutual information and logarithmic negativity, a relation that also holds for stabilizer states. For general tripartite pure states, they relate dihedral invariants to Rényi reflected entropies, demonstrating that dihedral permutations of replicas are equivalent to the reflected construction or realignment of density matrices.
Significance. If the central claims are substantiated with explicit derivations, the work would provide analytical tools for multipartite entanglement in Lifshitz theories with anisotropic scaling, which are relevant to certain condensed-matter systems. The explicit relations to mutual information, logarithmic negativity, and reflected entropies could enable cross-checks with established measures and extend replica techniques beyond relativistic CFTs. The analytic continuation to non-integer Rényi indices, if rigorously justified, would be a useful computational advance.
major comments (1)
- [Lifshitz ground states computation and analytic continuation] The central claim of an explicit computation of genuine multientropy for Lifshitz ground states together with its analytic continuation to non-integer Rényi index lacks displayed derivation steps, the explicit continued expression, pole locations, or regularization procedure. Given the anisotropic scaling z ≠ 1, which alters the replica manifold and twist-operator structure relative to relativistic cases, this omission prevents verification that the n → 1 limit remains a valid entanglement monotone. This issue is load-bearing for the main result stated in the abstract.
minor comments (1)
- The relation between genuine multientropy and mutual information plus logarithmic negativity is stated to hold for stabilizer states, but a brief explicit check or reference to the stabilizer case would improve readability.
Simulated Author's Rebuttal
We thank the referee for their careful reading of our manuscript and for providing constructive feedback. We are pleased that the referee recognizes the potential utility of our results for studying multipartite entanglement in Lifshitz theories. We address the major comment below.
read point-by-point responses
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Referee: The central claim of an explicit computation of genuine multientropy for Lifshitz ground states together with its analytic continuation to non-integer Rényi index lacks displayed derivation steps, the explicit continued expression, pole locations, or regularization procedure. Given the anisotropic scaling z ≠ 1, which alters the replica manifold and twist-operator structure relative to relativistic cases, this omission prevents verification that the n → 1 limit remains a valid entanglement monotone. This issue is load-bearing for the main result stated in the abstract.
Authors: We thank the referee for highlighting this important point. We agree that the derivation steps for the computation of genuine multientropy in Lifshitz ground states, together with the details of the analytic continuation, would benefit from a more explicit presentation to facilitate verification, particularly in light of the anisotropic scaling z ≠ 1 and its effects on the replica manifold and twist operators. In the revised manuscript, we will expand the relevant sections to include step-by-step derivations of the genuine multientropy for Lifshitz ground states. We will provide the explicit form of the analytically continued expression, discuss the locations of poles, and outline the regularization procedure. We will also elaborate on the validity of the n → 1 limit as an entanglement monotone, carefully addressing the modifications arising from the Lifshitz scaling. These revisions will strengthen the substantiation of our central claim. revision: yes
Circularity Check
Derivation of genuine multientropy and dihedral invariants is self-contained
full rationale
The paper derives the genuine multientropy for Lifshitz ground states via replica methods and obtains its analytic continuation in the Rényi index, then expresses it in terms of mutual information and logarithmic negativity. It further relates dihedral invariants to Rényi reflected entropies for general tripartite states. These steps are presented as explicit computations and equivalences rather than reductions to fitted parameters or prior self-definitions. No load-bearing self-citations or ansatzes imported from the authors' own work are required for the central results, and the relations hold independently for stabilizer states as an external check. The replica construction is invoked with the standard assumption that the continuation is well-defined, but this does not make the output equivalent to the input by construction.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Replica trick for Rényi entropies admits analytic continuation to non-integer index while preserving monotonicity properties.
- domain assumption Lifshitz ground states are pure tripartite states whose multi-copy invariants can be computed via standard quantum-field-theory techniques.
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We compute the (genuine) multientropy for Lifshitz groundstates... G(3)_n(A:B:C)=2-n/2n (I_{1/2}(A:B)-2E(A:B))
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IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
dihedral permutations of replicas are equivalent to the reflected construction
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Forward citations
Cited by 2 Pith papers
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The Junction Law for Multipartite Entanglement in Confining Holographic Backgrounds
The junction law for multipartite entanglement persists in confining holographic backgrounds, but phase structure and GM short-distance scaling (L^{-4}, L^{-2}, or L^{-2}(log L)^2) are background-dependent.
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Tripartite Correlation Signal from Multipartite Entanglement of Purification
Δ^(3)_p is a non-negative signal detecting genuine tripartite entanglement, extended via the E_w = E_p conjecture to holographic systems in AdS3/CFT2.
Reference graph
Works this paper leans on
-
[1]
On a finite interval a. DisjointA, Bin the bulk C1 A C2 B C3 ℓC1 ℓA ℓC2 ℓB ℓC3 M (3) 3 = φ 6 φ 12 φ 5 φ 11 φ 4 φ 10 φ 3 φ 9 φ 2 φ 8 φ 1 φ 7 FIG. A1. Disjoint regionsAandBin the bulk. Right: Replica graph resulting from the multi-entropy symmetry forn= 3. Multi-entropy— We begin by computing the multi-entropy for Dirichlet boundary conditions, and then bri...
-
[2]
DisjointA, B Multi-entropy— For disconnectedAandBon a circle (see Fig
On a circle a. DisjointA, B Multi-entropy— For disconnectedAandBon a circle (see Fig. A4), the partition function on the replica graph reads Z (3) n = Z dϕ1...dϕ4n nY i=1 K(ϕ 2i−1, ϕ2n+2i−1;ℓ A)nK(ϕ 2i, ϕ2n+2i;ℓ B)n × 2n−1Y j=1 K(ϕ j, ϕj+1;ℓ C1) 2n−j 2 −1 Y k=1 K(ϕ j, ϕj+2k+1;ℓ C1) × 2n−1Y l=1 K(ϕ 2n+l, ϕ2n+l+1;ℓ C2) 2n−l 2 −1 Y q=1 K(ϕ 2n+l, ϕ2n+l+2q+1;ℓ...
-
[3]
Alternative normalization and definition of dihedral invariant In defining the family of dihedral invariants (7), we chose a particular prescription for normalization. Though our choice appears natural since we prove that the dihedral invariant (7) is exactly the (2, n)–R´ enyi reflected entropy, see (40), it is interesting to explore other normalizations...
-
[4]
Dihedral invariant for pure tripartite qubit states We compute the dihedral invariant and reflected entropy of generalized GHZ and W states, and show that these two quantities are equivalent. a. GHZ states Consider the generalized GHZ state defined as |GHZ(θ)⟩= cosθ|000⟩+ sinθ|111⟩.(B5) Since this state is symmetric under qubit permutations, the dihedral ...
-
[5]
Disjoint regions on the boundary M D 2 = φ 1 φ 3 φ 4 φ 2 M D 3 = φ 1 φ 3 φ 4 φ 5 φ 2 FIG
Dihedral invariant for Lifshitz groundstates a. Disjoint regions on the boundary M D 2 = φ 1 φ 3 φ 4 φ 2 M D 3 = φ 1 φ 3 φ 4 φ 5 φ 2 FIG. B6. Replica graphs for the dihedral invariants of two disjoint regionsA, Bon the boundary (see Fig. 1(a)), forn= 2,3. For two disjoint regionsA, B, shown in Fig. 1(a), we illustrates the replica graph for two differentn...
-
[6]
Disjoint regions on the boundary Associated to the replica graph shown in Fig
Multi-entropy a. Disjoint regions on the boundary Associated to the replica graph shown in Fig. 2 is the following 2n×2nmatrix M (3) n = a c0c· · · c b c0c· · · c a c0c· · · ... ... ... ... ... · · ·c0c b c0 · · ·c0c a c · · ·c0c b ,(C2) wherea=nω coth(ωℓA) + coth(ωℓC) ,b=nω coth(ωℓB) + coth(ωℓC) andc=−ω/sinh(ωℓ C). Determinant— We...
-
[7]
Dihedral invariant a. Disjoint regions on the boundary The matrixM (D) n associated with the partition function of the dihedral invariant for this situation, see Fig. B7, is M (D) n = a0−c· · · · · · −c 0a−c· · · · · · −c −c−c b0· · ·0 ... ... 0 ... ... ... ... ... ... 0 −c−c0· · ·0b , a=nω coth(ωℓA) + coth(ωℓC) , b= 2ω coth(ωℓB) +...
-
[8]
Entanglement in Many-Body Systems
L. Amico, R. Fazio, A. Osterloh, and V. Vedral, “Entan- glement in many-body systems,”Rev. Mod. Phys.80, 517 (2008),arXiv:quant-ph/0703044
work page internal anchor Pith review Pith/arXiv arXiv 2008
-
[9]
Quantum entanglement in condensed matter systems
N. Laflorencie, “Quantum entanglement in con- densed matter systems,”Phys. Rept.646, 1 (2016), arXiv:1512.03388
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[10]
Entanglement in quantum critical phenomena
G. Vidal, J. I. Latorre, E. Rico, and A. Ki- taev, “Entanglement in quantum critical phe- nomena,”Phys. Rev. Lett.90, 227902 (2003), arXiv:quant-ph/0211074
work page internal anchor Pith review Pith/arXiv arXiv 2003
-
[11]
Entanglement Entropy and Quantum Field Theory
P. Calabrese and J. L. Cardy, “Entanglement entropy and quantum field theory,”J. Stat. Mech.0406, P06002 (2004),arXiv:hep-th/0405152
work page internal anchor Pith review Pith/arXiv arXiv 2004
-
[12]
Boundary Effects in the Critical Scaling of Entan- glement Entropy in 1D Systems,
N. Laflorencie, E. S. Sorensen, M.-S. Chang, and I. Af- fleck, “Boundary Effects in the Critical Scaling of Entan- glement Entropy in 1D Systems,”Phys. Rev. Lett.96, 100603 (2006)
work page 2006
-
[13]
Area laws for the entanglement entropy - a review
J. Eisert, M. Cramer, and M. B. Plenio, “Area laws for the entanglement entropy - a review,”Rev. Mod. Phys. 82, 277 (2010),arXiv:0808.3773
work page internal anchor Pith review Pith/arXiv arXiv 2010
-
[14]
Entanglement entropy in quantum impurity systems and systems with boundaries
I. Affleck, N. Laflorencie, and E. S. Sorensen, “Entangle- ment entropy in quantum impurity systems and systems with boundaries,”J. Phys. A: Math. Theor.42, 504009 (2009),arXiv:0906.1809
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[15]
Universality of corner entanglement in conformal field theories
P. Bueno, R. C. Myers, and W. Witczak-Krempa, “Universality of corner entanglement in conformal field theories,”Phys. Rev. Lett.115, 021602 (2015), arXiv:1505.04804
work page internal anchor Pith review Pith/arXiv arXiv 2015
-
[16]
Anomalies, entropy and boundaries
D. V. Fursaev and S. N. Solodukhin, “Anomalies, en- tropy and boundaries,”Phys. Rev.D93, 084021 (2016), arXiv:1601.06418
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[17]
The g-theorem and quantum information theory
H. Casini, I. S. Landea, and G. Torroba, “The g-theorem and quantum information theory,”JHEP10, 140 (2016), arXiv:1607.00390
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[18]
Boundary-corner entanglement for free bosons
C. Berthiere, “Boundary-corner entanglement for free bosons,”Phys. Rev. B99, 165113 (2019), arXiv:1811.12875
work page internal anchor Pith review Pith/arXiv arXiv 2019
-
[19]
Relating bulk to boundary entanglement,
C. Berthiere and W. Witczak-Krempa, “Relating bulk to boundary entanglement,”Phys. Rev. B100, 235112 (2019),arXiv:1907.11249
-
[20]
Entanglement of Skeletal Regions,
C. Berthiere and W. Witczak-Krempa, “Entanglement of Skeletal Regions,”Phys. Rev. Lett.128, 240502 (2022), arXiv:2112.13931
-
[21]
Topological entanglement entropy
A. Kitaev and J. Preskill, “Topological entangle- ment entropy,”Phys. Rev. Lett.96, 110404 (2006), arXiv:hep-th/0510092
work page internal anchor Pith review Pith/arXiv arXiv 2006
-
[22]
Detecting topological order in a ground state wave function
M. Levin and X.-G. Wen, “Detecting topological order in a ground state wave function,””Phys. Rev. Lett.”96, 110405 (2006),arXiv:cond-mat/0510613
work page internal anchor Pith review Pith/arXiv arXiv 2006
-
[23]
B. Zeng, X. Chen, D.-L. Zhou, and X.-G. Wen, “Quan- tum Information Meets Quantum Matter – From Quan- tum Entanglement to Topological Phase in Many-Body Systems,”arXiv:1508.02595
work page internal anchor Pith review Pith/arXiv arXiv
-
[24]
Holographic Entanglement Entropy
M. Rangamani and T. Takayanagi,Holographic En- tanglement Entropy, vol. 931. Springer, 2017. arXiv:1609.01287
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[25]
Takayanagi,Essay: Emergent Holographic Spacetime from Quantum Information,Phys
T. Takayanagi, “Essay: Emergent Holographic Space- time from Quantum Information,”Phys. Rev. Lett.134, 240001 (2025),arXiv:2506.06595
-
[26]
Entanglement Wedge Cross Sections Require Tripartite Entanglement,
C. Akers and P. Rath, “Entanglement Wedge Cross Sec- tions Require Tripartite Entanglement,”JHEP04, 208 (2020),arXiv:1911.07852
-
[27]
Universal tripartite entanglement in one-dimensional many-body systems,
Y. Zou, K. Siva, T. Soejima, R. S. K. Mong, and M. P. Zaletel, “Universal tripartite entanglement in one- dimensional many-body systems,”Phys. Rev. Lett.126, 120501 (2021),arXiv:2011.11864
-
[28]
The Markov gap for geometric reflected entropy,
P. Hayden, O. Parrikar, and J. Sorce, “The Markov gap for geometric reflected entropy,”JHEP10, 047 (2021), arXiv:2107.00009
-
[29]
Multipartitioning topological phases by vertex states and quantum entanglement,
Y. Liu, R. Sohal, J. Kudler-Flam, and S. Ryu, “Multipar- titioning topological phases by vertex states and quan- tum entanglement,”Phys. Rev. B105, 115107 (2022), 21 arXiv:2110.11980
-
[30]
Topological multipartite entanglement in a Fermi liquid,
P. M. Tam, M. Claassen, and C. L. Kane, “Topo- logical multipartite entanglement in a Fermi liquid,” Phys. Rev. X12, 031022 (2022),arXiv:2204.06559
-
[31]
Separability and entanglement of resonating valence-bond states
G. Parez, C. Berthiere, and W. Witczak-Krempa, “Separability and entanglement of resonating valence-bond states,”SciPost Phys.15, 066 (2023), arXiv:2212.11740
work page internal anchor Pith review Pith/arXiv arXiv 2023
-
[32]
Multipartite information of free fermions on hamming graphs,
G. Parez, P.-A. Bernard, N. Cramp´ e, and L. Vinet, “Multipartite information of free fermions on Ham- ming graphs,”Nucl. Phys. B990, 116157 (2023), arXiv:2212.09158
-
[33]
Multipartite entanglement in two-dimensional chiral topological liquids,
Y. Liu, Y. Kusuki, J. Kudler-Flam, R. Sohal, and S. Ryu, “Multipartite entanglement in two-dimensional chiral topological liquids,”Phys. Rev. B109, 085108 (2024), arXiv:2301.07130
-
[34]
Reflected entropy and Markov gap in Lifshitz theories,
C. Berthiere, B. Chen, and H. Chen, “Reflected entropy and Markov gap in Lifshitz theories,”JHEP09, 160 (2023),arXiv:2307.12247
-
[35]
G. Parez and W. Witczak-Krempa, “The Fate of Entan- glement,”arXiv:2402.06677
-
[36]
Separable ellipsoids around multi- partite states,
R. Y. Wen, G. Parez, L. Lyu, W. Witczak-Krempa, and A. Kempf, “Separable ellipsoids around multi- partite states,”Phys. Rev. A112, 012426 (2025), arXiv:2410.05400
-
[37]
Tripartite entanglement dynamics follow- ing a quantum quench,
C. Berthiere, “Tripartite entanglement dynamics follow- ing a quantum quench,”arXiv:2408.12533
- [38]
-
[39]
New multipartite entanglement measure and its holographic dual
A. Gadde, V. Krishna, and T. Sharma, “New multi- partite entanglement measure and its holographic dual,” Phys. Rev. D106, 126001 (2022),arXiv:2206.09723
-
[40]
G. Penington, M. Walter, and F. Witteveen, “Fun with replicas: tripartitions in tensor networks and gravity,” JHEP05, 008 (2023),arXiv:2211.16045
-
[41]
A canonical purification for the entanglement wedge cross-section
S. Dutta and T. Faulkner, “A canonical purification for the entanglement wedge cross-section,”JHEP03, 178 (2021),arXiv:1905.00577
work page internal anchor Pith review Pith/arXiv arXiv 2021
-
[42]
Computable Cross Norm in Tensor Networks and Holography,
A. Milekhin, P. Rath, and W. Weng, “Computable Cross Norm in Tensor Networks and Holography,” arXiv:2212.11978
-
[43]
Reflected entropy and com- putable cross-norm negativity: Free theories and sym- metry resolution,
C. Berthiere and G. Parez, “Reflected entropy and com- putable cross-norm negativity: Free theories and sym- metry resolution,”Phys. Rev. D108, 054508 (2023), arXiv:2307.11009
- [44]
-
[45]
N. Iizuka and M. Nishida, “Genuine multientropy and holography,”Phys. Rev. D112, 026011 (2025), arXiv:2502.07995
- [46]
- [47]
- [48]
-
[49]
Multi wavefunction overlap and multi en- tropy for topological ground states in (2+1) dimensions,
B. Liu, J. Zhang, S. Ohyama, Y. Kusuki, and S. Ryu, “Multi wavefunction overlap and multi en- tropy for topological ground states in (2+1) dimensions,” arXiv:2410.08284
-
[50]
Black hole multi- entropy curves — secret entanglement between Hawking particles,
N. Iizuka, S. Lin, and M. Nishida, “Black hole multi- entropy curves — secret entanglement between Hawking particles,”JHEP03, 037 (2025),arXiv:2412.07549
-
[51]
Why many- partite entanglement is essential for holography,
N. Iizuka, S. Lin, and M. Nishida, “Why many- partite entanglement is essential for holography,” arXiv:2504.01625
- [52]
- [53]
-
[54]
Superconductivity and the Quantum Hard-Core Dimer Gas,
D. S. Rokhsar and S. A. Kivelson, “Superconductivity and the Quantum Hard-Core Dimer Gas,”Phys. Rev. Lett.61, 2376–2379 (1988)
work page 1988
-
[55]
From classical to quantum dynamics at Rokhsar-Kivelson points
C. L. Henley, “From classical to quantum dynamics at rokhsar–kivelson points,”Journal of Physics: Condensed Matter16, S891 (2004),arXiv:cond-mat/0311345
work page internal anchor Pith review Pith/arXiv arXiv 2004
-
[56]
Entanglement and separability in continuum Rokhsar-Kivelson states,
C. Boudreault, C. Berthiere, and W. Witczak-Krempa, “Entanglement and separability in continuum Rokhsar- Kivelson states,”Phys. Rev. Res.4, 033251 (2022), arXiv:2110.04290
-
[57]
Entanglement entropy of 2D conformal quantum critical points: hearing the shape of a quantum drum
E. Fradkin and J. E. Moore, “Entanglement entropy of 2D conformal quantum critical points: hearing the shape of a quantum drum,”Phys. Rev. Lett.97, 050404 (2006), arXiv:cond-mat/0605683
work page internal anchor Pith review Pith/arXiv arXiv 2006
-
[58]
Universal entanglement entropy in 2D conformal quantum critical points
B. Hsu, M. Mulligan, E. Fradkin, and E.-A. Kim, “Universal entanglement entropy in 2D conformal quan- tum critical points,”Phys. Rev.B79, 115421 (2009), arXiv:0812.0203
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[59]
Shannon and entanglement entropies of one- and two-dimensional critical wave functions
J.-M. St´ ephan, S. Furukawa, G. Misguich, and V. Pasquier, “Shannon and entanglement entropies of one- and two-dimensional critical wave functions,” ”Phys. Rev. B”80, 184421 (2009),arXiv:0906.1153
work page internal anchor Pith review Pith/arXiv arXiv 2009
-
[60]
M. Oshikawa, “Boundary Conformal Field Theory and Entanglement Entropy in Two-Dimensional Quantum Lifshitz Critical Point,”arXiv:1007.3739
work page internal anchor Pith review Pith/arXiv arXiv
-
[61]
M. P. Zaletel, J. H. Bardarson, and J. E. Moore, “Logarithmic Terms in Entanglement Entropies of 2D Quantum Critical Points and Shannon Entropies of Spin Chains,”Phys. Rev. Lett.107, 020402 (2011), arXiv:1103.5452
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[62]
T. Zhou, X. Chen, T. Faulkner, and E. Fradkin, “En- tanglement entropy and mutual information of circular entangling surfaces in the 2 + 1-dimensional quantum Lifshitz model,”J. Stat. Mech.1609, 093101 (2016), arXiv:1607.01771
work page internal anchor Pith review Pith/arXiv arXiv 2016
-
[63]
Two-cylinder entanglement entropy under a twist
X. Chen, W. Witczak-Krempa, T. Faulkner, and E. Frad- kin, “Two-cylinder entanglement entropy under a twist,” J. Stat. Mech.1704, 043104 (2017),arXiv:1611.01847
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[64]
Quantum spin chains with multiple dynamics
X. Chen, E. Fradkin, and W. Witczak-Krempa, “Quan- tum spin chains with multiple dynamics,”Phys. Rev. B 96, 180402 (2017),arXiv:1706.02304
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[65]
Entanglement in Lifshitz-type Quantum Field Theories
M. R. Mohammadi Mozaffar and A. Mollabashi, “Entan- glement in Lifshitz-type Quantum Field Theories,”JHEP 07, 120 (2017),arXiv:1705.00483
work page internal anchor Pith review Pith/arXiv arXiv 2017
-
[66]
Logarithmic Negativity in Lifshitz Harmonic Models
M. R. Mohammadi Mozaffar and A. Mollabashi, “Loga- rithmic Negativity in Lifshitz Harmonic Models,”J. Stat. Mech.1805, 053113 (2018),arXiv:1712.03731
work page internal anchor Pith review Pith/arXiv arXiv 2018
-
[67]
Entanglement Entropy in Generalised Quantum Lifshitz Models,
J. Angel-Ramelli, V. G. M. Puletti, and L. Thorlacius, “Entanglement Entropy in Generalised Quantum Lifshitz Models,”JHEP08, 072 (2019),arXiv:1906.08252
-
[68]
Logarithmic Negativity in Quantum Lifshitz Theories,
J. Angel-Ramelli, C. Berthiere, V. G. M. Puletti, and L. Thorlacius, “Logarithmic Negativity in Quan- 22 tum Lifshitz Theories,”JHEP09, 011 (2020), arXiv:2002.05713
-
[69]
Entanglement Entropy of Excited States in the Quantum Lifshitz Model,
J. Angel-Ramelli, “Entanglement Entropy of Excited States in the Quantum Lifshitz Model,”J. Stat. Mech. 2101, 013102 (2021),arXiv:2009.02283
-
[70]
A computable measure of entanglement
G. Vidal and R. F. Werner, “Computable measure of entanglement,”Phys. Rev.A65, 032314 (2002), arXiv:quant-ph/0102117
work page internal anchor Pith review Pith/arXiv arXiv 2002
-
[71]
Separability Criterion for Density Matrices
A. Peres, “Separability criterion for density matrices,”Phys. Rev. Lett.77, 1413 (1996), arXiv:quant-ph/9604005
work page internal anchor Pith review Pith/arXiv arXiv 1996
-
[72]
Reflected Entropy and Entanglement Wedge Cross Section with the First Order Correction,
H.-S. Jeong, K.-Y. Kim, and M. Nishida, “Reflected Entropy and Entanglement Wedge Cross Section with the First Order Correction,”JHEP12, 170 (2019), arXiv:1909.02806
-
[73]
Reflected entropy, sym- metries and free fermions,
P. Bueno and H. Casini, “Reflected entropy, sym- metries and free fermions,”JHEP05, 103 (2020), arXiv:2003.09546
-
[74]
Reflected Entropy for an Evaporating Black Hole,
T. Li, J. Chu, and Y. Zhou, “Reflected Entropy for an Evaporating Black Hole,”JHEP11, 155 (2020), arXiv:2006.10846
-
[75]
Topological reflected entropy in Chern-Simons theories,
C. Berthiere, H. Chen, Y. Liu, and B. Chen, “Topological reflected entropy in Chern-Simons theories,”Phys. Rev. B103, 035149 (2021),arXiv:2008.07950
-
[76]
Reflected entropy for free scalars,
P. Bueno and H. Casini, “Reflected entropy for free scalars,”JHEP11, 148 (2020),arXiv:2008.11373
-
[77]
The Page curve for reflected entropy,
C. Akers, T. Faulkner, S. Lin, and P. Rath, “The Page curve for reflected entropy,”JHEP06, 089 (2022), arXiv:2201.11730
-
[78]
Reflected en- tropy in AdS 3/WCFT,
B. Chen, Y. Liu, and B. Yu, “Reflected en- tropy in AdS 3/WCFT,”JHEP12, 008 (2022), arXiv:2205.05582
-
[79]
Holographic study of reflected entropy in anisotropic theories,
M. J. Vasli, M. R. Mohammadi Mozaffar, K. Babaei Velni, and M. Sahraei, “Holographic study of reflected entropy in anisotropic theories,”Phys. Rev. D 107, 026012 (2023),arXiv:2207.14169
-
[80]
The Markov gap in the presence of islands,
Y. Lu and J. Lin, “The Markov gap in the presence of islands,”JHEP03, 043 (2023),arXiv:2211.06886
discussion (0)
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