pith. sign in

arxiv: 2509.22051 · v2 · submitted 2025-09-26 · ❄️ cond-mat.str-el · hep-th· math-ph· math.MP

From gauging to duality in one-dimensional quantum lattice models

Pith reviewed 2026-05-18 13:09 UTC · model grok-4.3

classification ❄️ cond-mat.str-el hep-thmath-phmath.MP
keywords gaugingdualitymatrix product operatorsone-dimensional modelsquantum symmetriescategorical symmetriesbackground fields
0
0 comments X p. Extension

The pith

Gauging and duality transformations are equivalent up to constant depth quantum circuits in one-dimensional quantum lattice models.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper demonstrates that gauging and duality transformations are equivalent up to constant depth quantum circuits in one-dimensional quantum lattice models. This equivalence is shown using matrix product operators that act as the lattice representation theory for global categorical symmetries and classify duality transformations. A sympathetic reader would care because these tools are central to understanding symmetries in many-body physics, and their equivalence can simplify analysis of quantum phases and allow clearer handling of background fields. The construction makes the symmetries of the gauged theory manifest.

Core claim

Gauging and duality transformations are shown to be equivalent up to constant depth quantum circuits in the case of one-dimensional quantum lattice models. This is demonstrated by making use of matrix product operators, which provide the lattice representation theory for global (categorical) symmetries as well as a classification of duality transformations. The construction makes the symmetries of the gauged theory manifest and clarifies how to deal with static background fields when gauging generalised symmetries.

What carries the argument

Matrix product operators providing the lattice representation theory for global categorical symmetries and a classification of duality transformations.

If this is right

  • The symmetries of the gauged theory are made manifest.
  • Static background fields can be handled when gauging generalised symmetries.
  • Gauging and duality can be interchanged using only constant depth quantum circuits.
  • Duality transformations are classified within the same framework as symmetries.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • This equivalence may allow for easier construction of dual models in 1D by using gauging procedures.
  • It could be tested in specific models like spin chains to confirm the constant depth.
  • Connections to higher-dimensional models might reveal where this equivalence breaks down.

Load-bearing premise

Matrix product operators provide the lattice representation theory for global (categorical) symmetries as well as a classification of duality transformations.

What would settle it

A calculation in a concrete 1D model such as the Ising chain showing that the gauged and dual versions require a circuit depth greater than constant to be related.

read the original abstract

Gauging and duality transformations, two of the most useful tools in many-body physics, are shown to be equivalent up to constant depth quantum circuits in the case of one-dimensional quantum lattice models. This is demonstrated by making use of matrix product operators, which provide the lattice representation theory for global (categorical) symmetries as well as a classification of duality transformations. Our construction makes the symmetries of the gauged theory manifest and clarifies how to deal with static background fields when gauging generalised symmetries.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The paper claims that gauging and duality transformations are equivalent up to constant-depth quantum circuits for one-dimensional quantum lattice models. This equivalence is demonstrated by employing matrix product operators (MPOs), which serve as the lattice representation theory for global categorical symmetries and provide a classification of duality transformations. The construction renders the symmetries of the gauged theory manifest and clarifies the treatment of static background fields for generalized symmetries.

Significance. If the central claim is established rigorously, the result unifies two foundational tools in many-body physics at the lattice level for 1D systems with generalized symmetries. The MPO-based approach supplies a concrete representation-theoretic foundation that could streamline constructions of symmetry-enriched phases and duality maps, with potential implications for quantum simulation and topological order. The explicit handling of background fields is a useful practical contribution.

major comments (1)
  1. The central claim equates gauging with duality via constant-depth circuits by invoking MPOs as both the lattice representation theory for categorical symmetries and the classifier of dualities. This step is load-bearing because an MPO with fixed bond dimension still requires an explicit decomposition into a depth-O(1) quantum circuit (independent of chain length L) whose gates implement the duality map while preserving the gauged theory's symmetries. If the construction only shows an abstract MPO correspondence without proving that the circuit depth remains bounded when the symmetry category is non-invertible or when static background fields are included, the equivalence fails to hold beyond invertible cases.
minor comments (2)
  1. Notation for the MPO bond dimension and its relation to the symmetry category should be introduced earlier and used consistently throughout the derivations.
  2. A brief comparison table or explicit example contrasting the new construction with prior invertible-symmetry results would improve readability.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for recognizing the potential unifying implications of the MPO-based approach. We address the major comment below and will incorporate clarifications to strengthen the presentation of the circuit decomposition.

read point-by-point responses
  1. Referee: The central claim equates gauging with duality via constant-depth circuits by invoking MPOs as both the lattice representation theory for categorical symmetries and the classifier of dualities. This step is load-bearing because an MPO with fixed bond dimension still requires an explicit decomposition into a depth-O(1) quantum circuit (independent of chain length L) whose gates implement the duality map while preserving the gauged theory's symmetries. If the construction only shows an abstract MPO correspondence without proving that the circuit depth remains bounded when the symmetry category is non-invertible or when static background fields are included, the equivalence fails to hold beyond invertible cases.

    Authors: We thank the referee for this precise and load-bearing observation. In the manuscript the duality map is realized by an MPO whose bond dimension is fixed solely by the data of the symmetry category (or fusion category) and is therefore independent of system size L. In one dimension any such fixed-bond-dimension MPO admits an exact decomposition into a quantum circuit of depth O(1) (with the constant set by the bond dimension and the local Hilbert-space dimension). The decomposition proceeds by sequentially applying local unitary gates that realize the MPO tensors; because the number of layers needed to contract or implement the MPO is bounded by the bond dimension, the circuit depth remains independent of L. The same construction applies verbatim to non-invertible symmetries, since the categorical structure is already encoded in the fixed bond dimension and the fusion rules of the MPO. Static background fields are incorporated as fixed, finite-support defects or insertions into the MPO tensors; these defects do not increase the bond dimension and can be absorbed into the same constant-depth circuit without additional layers. We will add a new subsection (and an accompanying figure) that explicitly carries out the MPO-to-circuit conversion for both an invertible and a non-invertible example, including the case with a non-trivial background field, thereby making the depth bound fully rigorous. revision: yes

Circularity Check

0 steps flagged

Minor self-citation risk from established MPO framework; central equivalence claim remains independent

full rationale

The derivation uses matrix product operators to represent categorical symmetries and classify dualities, then constructs an explicit equivalence to gauging via constant-depth circuits while making symmetries manifest and handling background fields. This builds on prior tensor-network literature (including work by overlapping authors) but does not reduce the main result to a self-referential definition, a fitted parameter renamed as prediction, or an unverified uniqueness theorem. The construction supplies new content by linking gauging directly to duality maps in 1D lattices, remaining self-contained against external benchmarks in MPO theory and quantum circuit depth analysis. No load-bearing step collapses to its own inputs by construction.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the domain assumption that matrix product operators furnish a complete representation theory and duality classification for 1D lattice symmetries; no explicit free parameters or new entities are identified from the abstract.

axioms (1)
  • domain assumption Matrix product operators provide the lattice representation theory for global (categorical) symmetries as well as a classification of duality transformations.
    Invoked in the abstract as the key technical tool enabling the equivalence proof.

pith-pipeline@v0.9.0 · 5634 in / 1248 out tokens · 52287 ms · 2026-05-18T13:09:45.473196+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

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 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Continuum limit of gauged tensor network states

    hep-th 2025-11 unverdicted novelty 6.0

    The continuum limit of gauged tensor networks is well defined and produces a new class of states for non-perturbative continuum gauge theories.

Reference graph

Works this paper leans on

81 extracted references · 81 canonical work pages · cited by 1 Pith paper · 26 internal anchors

  1. [1]

    Aasen, P

    D. Aasen, P. Fendley, and R. S. K. Mong, Topological Defects on the Lattice: Dualities and Degeneracies , http://arxiv.org/abs/2008.08598 arXiv:2008.08598 [cond-mat.stat-mech]

  2. [2]

    Asaeda and U

    M. Asaeda and U. Haagerup, Exotic subfactors of finite depth with Jones indices (5+ 13 )/2 and (5+ 17 )/2 , http://dx.doi.org/https://doi.org/10.1007/s002200050574 Communications in mathematical physics 202 (1999) 1--63

  3. [3]

    Topological Defects on the Lattice I: The Ising model

    D. Aasen, R. S. K. Mong, and P. Fendley, Topological Defects on the Lattice I: The Ising model , http://dx.doi.org/10.1088/1751-8113/49/35/354001 J. Phys. A 49 (2016) 354001 , http://arxiv.org/abs/1601.07185 arXiv:1601.07185 [cond-mat.stat-mech]

  4. [4]

    Buerschaper, M

    O. Buerschaper, M. Aguado, and G. Vidal, Explicit tensor network representation for the ground states of string-net models, Phys. Rev. B 79 (2009) 085119 https://link.aps.org/doi/10.1103/PhysRevB.79.085119

  5. [5]

    Barter, J

    D. Barter, J. C. Bridgeman, and R. Wolf, Computing associators of endomorphism fusion categories , SciPost Phys. 13 (2022) 029 https://scipost.org/10.21468/SciPostPhys.13.2.029

  6. [6]

    Y. BenTov, Fermion masses without symmetry breaking in two spacetime dimensions , http://dx.doi.org/10.1007/JHEP07(2015)034 JHEP 07 (2015) 034 , http://arxiv.org/abs/1412.0154 arXiv:1412.0154 [cond-mat.str-el]

  7. [7]

    Anyonic Chains, Topological Defects, and Conformal Field Theory

    M. Buican and A. Gromov, Anyonic Chains, Topological Defects, and Conformal Field Theory , http://dx.doi.org/10.1007/s00220-017-2995-6 Commun. Math. Phys. 356 (2017) 1017--1056 , http://arxiv.org/abs/1701.02800 arXiv:1701.02800 [hep-th]

  8. [8]

    J. C. Bridgeman, L. Lootens, and F. Verstraete, Invertible Bimodule Categories and Generalized Schur Orthogonality , http://dx.doi.org/10.1007/s00220-023-04781-y Commun. Math. Phys. 402 (2023) 2691--2714 , http://arxiv.org/abs/2211.01947 arXiv:2211.01947 [math.QA]

  9. [9]

    Anyons and matrix product operator algebras

    N. Bultinck, M. Mari\"en, D. J. Williamson, M. B. S ahino g lu, J. Haegeman, and F. Verstraete, Anyons and matrix product operator algebras , http://dx.doi.org/10.1016/j.aop.2017.01.004 Annals Phys. 378 (2017) 183--233 , http://arxiv.org/abs/1511.08090 arXiv:1511.08090 [cond-mat.str-el]

  10. [10]

    L. E. Bottini and S. Schafer-Nameki, A Gapless Phase with Haagerup Symmetry , http://arxiv.org/abs/2410.19040 arXiv:2410.19040 [hep-th]

  11. [11]

    Bhardwaj and Y

    L. Bhardwaj and Y. Tachikawa, On finite symmetries and their gauging in two dimensions , http://dx.doi.org/10.1007/JHEP03(2018)189 JHEP 03 (2018) 189 , http://arxiv.org/abs/1704.02330 arXiv:1704.02330 [hep-th]

  12. [12]

    Chatterjee, O

    A. Chatterjee, O. M. Aksoy, and X.-G. Wen, Quantum phases and transitions in spin chains with non-invertible symmetries , http://dx.doi.org/10.21468/SciPostPhys.17.4.115 SciPost Phys. 17 (2024) 115 , http://arxiv.org/abs/2405.05331 arXiv:2405.05331 [cond-mat.str-el]

  13. [13]

    Corcoran and M

    L. Corcoran and M. de Leeuw, Integrable and critical Haagerup spin chains , http://arxiv.org/abs/2410.16356 arXiv:2410.16356 [cond-mat.stat-mech]

  14. [14]

    2D symmetry protected topological orders and their protected gapless edge excitations

    X. Chen, Z.-X. Liu, and X.-G. Wen, Two-dimensional symmetry-protected topological orders and their protected gapless edge excitations , http://dx.doi.org/10.1103/PhysRevB.84.235141 Phys. Rev. B 84 (2011) 235141 , http://arxiv.org/abs/1106.4752 arXiv:1106.4752 [cond-mat.str-el]

  15. [15]

    Martín-Rodero and A

    E. Cobanera, G. Ortiz, and Z. Nussinov, The Bond-Algebraic Approach to Dualities , http://dx.doi.org/10.1080/00018732.2011.619814 Adv. Phys. 60 (2011) 679--798 , http://arxiv.org/abs/1103.2776 arXiv:1103.2776 [cond-mat.stat-mech]

  16. [16]

    Orbifold completion of defect bicategories

    N. Carqueville and I. Runkel, Orbifold completion of defect bicategories , http://dx.doi.org/10.4171/qt/76 Quantum Topol. 7 (2016) 203--279 , http://arxiv.org/abs/1210.6363 arXiv:1210.6363 [math.QA]

  17. [17]

    `Gauging' time reversal symmetry in tensor network states

    X. Chen and A. Vishwanath, Towards Gauging Time-Reversal Symmetry: A Tensor Network Approach , http://dx.doi.org/10.1103/PhysRevX.5.041034 Phys. Rev. X 5 (2015) 041034 , http://arxiv.org/abs/1401.3736 arXiv:1401.3736 [cond-mat.str-el]

  18. [18]

    M. B. S ahino g lu, D. Williamson, N. Bultinck, M. Mari\"en, J. Haegeman, N. Schuch, and F. Verstraete, Characterizing Topological Order with Matrix Product Operators , http://dx.doi.org/10.1007/s00023-020-00992-4 Annales Henri Poincare 22 (2021) 563--592 , http://arxiv.org/abs/1409.2150 arXiv:1409.2150 [quant-ph]

  19. [19]

    Diatlyk, C

    O. Diatlyk, C. Luo, Y. Wang, and Q. Weller, Gauging non-invertible symmetries: topological interfaces and generalized orbifold groupoid in 2d QFT , http://dx.doi.org/10.1007/JHEP03(2024)127 JHEP 03 (2024) 127 , http://arxiv.org/abs/2311.17044 arXiv:2311.17044 [hep-th]

  20. [20]

    Delcamp and A

    C. Delcamp and A. Tiwari, Higher categorical symmetries and gauging in two-dimensional spin systems , http://dx.doi.org/10.21468/SciPostPhys.16.4.110 SciPost Phys. 16 (2024) 110 , http://arxiv.org/abs/2301.01259 arXiv:2301.01259 [hep-th]

  21. [21]

    Etingof, S

    P. Etingof, S. Gelaki, D. Nikshych, and V. Ostrik, Tensor categories, American Mathematical Society, 2015

  22. [22]

    Fusion categories and homotopy theory

    P. Etingof, D. Nikshych, V. Ostrik, and w. a. a. b. E. Meir, Fusion categories and homotopy theory , http://arxiv.org/abs/0909.3140 arXiv:0909.3140 [math.QA]

  23. [23]

    D. S. Freed, G. W. Moore, and C. Teleman, Topological symmetry in quantum field theory , http://arxiv.org/abs/2209.07471 arXiv:2209.07471 [hep-th]

  24. [24]

    Franco-Rubio, A

    A. Franco-Rubio, A. Bochniak, and J. I. Cirac, Symmetry defects and gauging for quantum states with matrix product unitary symmetries , http://arxiv.org/abs/2502.20257 arXiv:2502.20257 [quant-ph]

  25. [25]

    TFT construction of RCFT correlators I: Partition functions

    J. Fuchs, I. Runkel, and C. Schweigert, TFT construction of RCFT correlators 1. Partition functions , http://dx.doi.org/10.1016/S0550-3213(02)00744-7 Nucl. Phys. B 646 (2002) 353--497 , http://arxiv.org/abs/hep-th/0204148 arXiv:hep-th/0204148

  26. [26]

    TFT construction of RCFT correlators II: Unoriented world sheets

    J. Fuchs, I. Runkel, and C. Schweigert, TFT construction of RCFT correlators. 2. Unoriented world sheets , http://dx.doi.org/10.1016/j.nuclphysb.2003.11.026 Nucl. Phys. B 678 (2004) 511--637 , http://arxiv.org/abs/hep-th/0306164 arXiv:hep-th/0306164

  27. [27]

    TFT construction of RCFT correlators III: Simple currents

    J. Fuchs, I. Runkel, and C. Schweigert, TFT construction of RCFT correlators. 3. Simple currents , http://dx.doi.org/10.1016/j.nuclphysb.2004.05.014 Nucl. Phys. B 694 (2004) 277--353 , http://arxiv.org/abs/hep-th/0403157 arXiv:hep-th/0403157

  28. [28]

    Interacting anyons in topological quantum liquids: The golden chain

    A. Feiguin, S. Trebst, A. W. W. Ludwig, M. Troyer, A. Kitaev, Z. Wang, and M. H. Freedman, Interacting anyons in topological quantum liquids: The golden chain , http://dx.doi.org/10.1103/PhysRevLett.98.160409 Phys. Rev. Lett. 98 (2007) 160409 , http://arxiv.org/abs/cond-mat/0612341 arXiv:cond-mat/0612341

  29. [29]

    Generalized Global Symmetries

    D. Gaiotto, A. Kapustin, N. Seiberg, and B. Willett, Generalized Global Symmetries , http://dx.doi.org/10.1007/JHEP02(2015)172 JHEP 02 (2015) 172 , http://arxiv.org/abs/1412.5148 arXiv:1412.5148 [hep-th]

  30. [30]

    Garre-Rubio and I

    J. Garre-Rubio and I. Kull, Gauging quantum states with nonanomalous matrix product operator symmetries , http://dx.doi.org/10.1103/PhysRevB.107.075137 Phys. Rev. B 107 (2023) 075137 , http://arxiv.org/abs/2209.07355 arXiv:2209.07355 [quant-ph]

  31. [31]

    Garre-Rubio, L

    J. Garre-Rubio, L. Lootens, and A. Moln \'a r, Classifying phases protected by matrix product operator symmetries using matrix product states , http://dx.doi.org/10.22331/q-2023-02-21-927 Quantum 7 (2023) 927 , http://arxiv.org/abs/2203.12563 arXiv:2203.12563 [cond-mat.str-el]

  32. [32]

    Grossman and N

    P. Grossman and N. Snyder, Quantum subgroups of the haagerup fusion categories, Communications in Mathematical Physics 311 (2012) 617–643 http://dx.doi.org/10.1007/s00220-012-1427-x

  33. [33]

    Haagerup, Principal graphs of subfactors in the index range 4<[m:n]< 3+ 2 , http://dx.doi.org/https://doi.org/10.1142/2394 Subfactors (1994)

    U. Haagerup, Principal graphs of subfactors in the index range 4<[m:n]< 3+ 2 , http://dx.doi.org/https://doi.org/10.1142/2394 Subfactors (1994)

  34. [34]

    Topological conformal defects with tensor networks

    M. Hauru, G. Evenbly, W. W. Ho, D. Gaiotto, and G. Vidal, Topological conformal defects with tensor networks , http://dx.doi.org/10.1103/PhysRevB.94.115125 Phys. Rev. B 94 (2016) 115125 , http://arxiv.org/abs/1512.03846 arXiv:1512.03846 [cond-mat.str-el]

  35. [35]

    Huang and Y.-H

    T.-C. Huang and Y.-H. Lin, The F -Symbols for Transparent Haagerup-Izumi Categories with G = Z _ 2n+1 , http://arxiv.org/abs/2007.00670 arXiv:2007.00670 [math.CT]

  36. [36]

    Huang, Y.-H

    T.-C. Huang, Y.-H. Lin, K. Ohmori, Y. Tachikawa, and M. Tezuka, Numerical evidence for a haagerup conformal field theory, Phys. Rev. Lett. 128 (2022) 231603 https://link.aps.org/doi/10.1103/PhysRevLett.128.231603

  37. [37]

    Diagonalizing transfer matrices and matrix product operators: a medley of exact and computational methods

    J. Haegeman and F. Verstraete, Diagonalizing Transfer Matrices and Matrix Product Operators: A Medley of Exact and Computational Methods , http://dx.doi.org/10.1146/annurev-conmatphys-031016-025507 Ann. Rev. Condensed Matter Phys. 8 (2017) 355--406 , http://arxiv.org/abs/1611.08519 arXiv:1611.08519 [cond-mat.str-el]

  38. [38]

    Haegeman, K

    J. Haegeman, K. Van Acoleyen, N. Schuch, J. I. Cirac, and F. Verstraete, Gauging quantum states: From global to local symmetries in many-body systems, Phys. Rev. X 5 (2015) 011024 https://link.aps.org/doi/10.1103/PhysRevX.5.011024

  39. [39]

    Jia, Quantum Cluster State Model with Haagerup Fusion Category Symmetry , http://arxiv.org/abs/2412.19657 arXiv:2412.19657 [math.QA]

    Z. Jia, Quantum Cluster State Model with Haagerup Fusion Category Symmetry , http://arxiv.org/abs/2412.19657 arXiv:2412.19657 [math.QA]

  40. [40]

    V. F. Jones, von Neumann algebras in mathematics and physics , American Mathematical Society, 1990

  41. [41]

    Jones, DHR bimodules of quasi-local algebras and symmetric quantum cellular automata , http://arxiv.org/abs/2304.00068 arXiv:2304.00068 [math-ph]

    C. Jones, DHR bimodules of quasi-local algebras and symmetric quantum cellular automata , http://arxiv.org/abs/2304.00068 arXiv:2304.00068 [math-ph]

  42. [42]

    Symmetric tensor networks and practical simulation algorithms to sharply identify classes of quantum phases distinguishable by short-range physics

    S. Jiang and Y. Ran, Symmetric tensor networks and practical simulation algorithms to sharply identify classes of quantum phases distinguishable by short-range physics, Phys. Rev. B 92 (2015) 104414 https://link.aps.org/doi/10.1103/PhysRevB.92.104414, http://arxiv.org/abs/1505.03171 arXiv:1505.03171 [cond-mat.str-el]

  43. [43]

    Jones, K

    C. Jones, K. Schatz, and D. J. Williamson, Quantum cellular automata and categorical dualities of spin chains , http://arxiv.org/abs/2410.08884 arXiv:2410.08884 [math-ph]

  44. [44]

    & Wigner, E

    P. Jordan and E. P. Wigner, About the Pauli exclusion principle , http://dx.doi.org/10.1007/BF01331938 Z. Phys. 47 (1928) 631--651

  45. [45]

    Anyons in an exactly solved model and beyond

    A. Kitaev, Anyons in an exactly solved model and beyond , http://dx.doi.org/10.1016/j.aop.2005.10.005 Annals Phys. 321 (2006) 2--111 , http://arxiv.org/abs/cond-mat/0506438 arXiv:cond-mat/0506438

  46. [46]

    Komargodski, K

    Z. Komargodski, K. Ohmori, K. Roumpedakis, and S. Seifnashri, Symmetries and strings of adjoint QCD _ 2 , http://dx.doi.org/10.1007/JHEP03(2021)103 JHEP 03 (2021) 103 , http://arxiv.org/abs/2008.07567 arXiv:2008.07567 [hep-th]

  47. [47]

    Kennedy and H

    T. Kennedy and H. Tasaki, Hidden Z2 Z2 symmetry breaking in Haldane-gap antiferromagnets , http://dx.doi.org/10.1103/PhysRevB.45.304 Phys. Rev. B 45 (1992) 304

  48. [48]

    H. A. Kramers and G. H. Wannier, Statistics of the two-dimensional ferromagnet. Part 1. , http://dx.doi.org/10.1103/PhysRev.60.252 Phys. Rev. 60 (1941) 252--262

  49. [49]

    Lootens, C

    L. Lootens, C. Delcamp, G. Ortiz, and F. Verstraete, Dualities in one-dimensional quantum lattice models: Symmetric hamiltonians and matrix product operator intertwiners, PRX Quantum 4 (2023) 020357 https://link.aps.org/doi/10.1103/PRXQuantum.4.020357

  50. [50]

    Lootens, C

    L. Lootens, C. Delcamp, and F. Verstraete, Dualities in one-dimensional quantum lattice models: Topological sectors, PRX Quantum 5 (2024) 010338 https://link.aps.org/doi/10.1103/PRXQuantum.5.010338

  51. [51]

    Lootens, C

    L. Lootens, C. Delcamp, and F. Verstraete, Entanglement and the density matrix renormalization group in the generalized landau paradigm, Nature Physics (2025) 1--7

  52. [52]

    Lootens, C

    L. Lootens, C. Delcamp, D. Williamson, and F. Verstraete, Low-depth unitary quantum circuits for dualities in one-dimensional quantum lattice models , http://arxiv.org/abs/2311.01439 arXiv:2311.01439 [quant-ph]

  53. [53]

    Lootens, J

    L. Lootens, J. Fuchs, J. Haegeman, C. Schweigert, and F. Verstraete, Matrix product operator symmetries and intertwiners in string-nets with domain walls , http://dx.doi.org/10.21468/SciPostPhys.10.3.053 SciPost Phys. 10 (2021) 053 , http://arxiv.org/abs/2008.11187 arXiv:2008.11187 [quant-ph]

  54. [54]

    L. Li, M. Oshikawa, and Y. Zheng, Noninvertible duality transformation between symmetry-protected topological and spontaneous symmetry breaking phases , http://dx.doi.org/10.1103/PhysRevB.108.214429 Phys. Rev. B 108 (2023) 214429 , http://arxiv.org/abs/2301.07899 arXiv:2301.07899 [cond-mat.str-el]

  55. [55]

    D.-C. Lu, Z. Sun, and Y.-Z. You, Realizing triality and p -ality by lattice twisted gauging in (1+1)d quantum spin systems , http://dx.doi.org/10.21468/SciPostPhys.17.5.136 SciPost Phys. 17 (2024) 136 , http://arxiv.org/abs/2405.14939 arXiv:2405.14939 [cond-mat.str-el]

  56. [56]

    Lootens, B

    L. Lootens, B. Vancraeynest-De Cuiper, N. Schuch, and F. Verstraete, Mapping between Morita-equivalent string-net states with a constant depth quantum circuit , http://dx.doi.org/10.1103/PhysRevB.105.085130 Phys. Rev. B 105 (2022) 085130 , http://arxiv.org/abs/2112.12757 arXiv:2112.12757 [quant-ph]

  57. [57]

    Moradi, O

    H. Moradi, O. M. Aksoy, J. H. Bardarson, and A. Tiwari, Symmetry fractionalization, mixed-anomalies and dualities in quantum spin models with generalized symmetries , http://arxiv.org/abs/2307.01266 arXiv:2307.01266 [cond-mat.str-el]

  58. [58]

    Moradi, S

    H. Moradi, S. F. Moosavian, and A. Tiwari, Topological holography: Towards a unification of Landau and beyond-Landau physics , http://dx.doi.org/10.21468/SciPostPhysCore.6.4.066 SciPost Phys. Core 6 (2023) 066 , http://arxiv.org/abs/2207.10712 arXiv:2207.10712 [cond-mat.str-el]

  59. [59]

    Neshveyev and M

    S. Neshveyev and M. Yamashita, A few remarks on the tube algebra of a monoidal category, http://dx.doi.org/10.1017/S0013091517000426 Proceedings of the Edinburgh Mathematical Society 61 (2018) 735–758

  60. [60]

    M. Oshikawa, Hidden Z_2 Z_2 symmetry in quantum spin chains with arbitrary integer spin , Journal of Physics: Condensed Matter 4 (1992) 7469 https://dx.doi.org/10.1088/0953-8984/4/36/019

  61. [61]

    Module categories, weak Hopf algebras and modular invariants

    V. Ostrik, Module categories, weak Hopf algebras and modular invariants , http://dx.doi.org/10.1007/s00031-003-0515-6 Transform. Groups 8 (2003) 177--206 , http://arxiv.org/abs/math/0111139 arXiv:math/0111139

  62. [62]

    T. J. Osborne, D. E. Stiegemann, and R. Wolf, The F-Symbols for the H3 Fusion Category , http://arxiv.org/abs/1906.01322 arXiv:1906.01322 [math.CT]

  63. [63]

    V. B. Petkova and J. B. Zuber, Generalized twisted partition functions , http://dx.doi.org/10.1016/S0370-2693(01)00276-3 Phys. Lett. B 504 (2001) 157--164 , http://arxiv.org/abs/hep-th/0011021 arXiv:hep-th/0011021

  64. [64]

    Spin Structures and Exact Dualities in Low Dimensions

    D. Radicevic, Spin Structures and Exact Dualities in Low Dimensions , http://arxiv.org/abs/1809.07757 arXiv:1809.07757 [hep-th]

  65. [65]

    Schaumann, Traces on module categories over fusion categories, Journal of Algebra 379 (2013) 382--425 https://www.sciencedirect.com/science/article/pii/S0021869313000380

    G. Schaumann, Traces on module categories over fusion categories, Journal of Algebra 379 (2013) 382--425 https://www.sciencedirect.com/science/article/pii/S0021869313000380

  66. [66]

    What's Done Cannot Be Undone: TASI Lectures on Non-Invertible Symmetries

    S.-H. Shao, What's Done Cannot Be Undone: TASI Lectures on Non-Invertible Symmetries , http://arxiv.org/abs/2308.00747 arXiv:2308.00747 [hep-th]

  67. [67]

    ICTP Lectures on (Non-)Invertible Generalized Symmetries

    S. Schafer-Nameki, ICTP lectures on (non-)invertible generalized symmetries , http://dx.doi.org/10.1016/j.physrep.2024.01.007 Phys. Rept. 1063 (2024) 1--55 , http://arxiv.org/abs/2305.18296 arXiv:2305.18296 [hep-th]

  68. [68]

    Seifnashri and S.-H

    S. Seifnashri and S.-H. Shao, Cluster State as a Noninvertible Symmetry-Protected Topological Phase , http://dx.doi.org/10.1103/PhysRevLett.133.116601 Phys. Rev. Lett. 133 (2024) 116601 , http://arxiv.org/abs/2404.01369 arXiv:2404.01369 [cond-mat.str-el]

  69. [69]

    Seiberg, S

    N. Seiberg, S. Seifnashri, and S.-H. Shao, Non-invertible symmetries and LSM-type constraints on a tensor product Hilbert space , http://dx.doi.org/10.21468/SciPostPhys.16.6.154 SciPost Phys. 16 (2024) 154 , http://arxiv.org/abs/2401.12281 arXiv:2401.12281 [cond-mat.str-el]

  70. [70]

    Seifnashri, S.-H

    S. Seifnashri, S.-H. Shao, and X. Yang, Gauging non-invertible symmetries on the lattice , http://dx.doi.org/10.21468/SciPostPhys.19.2.063 SciPost Phys. 19 (2025) 063 , http://arxiv.org/abs/2503.02925 arXiv:2503.02925 [cond-mat.str-el]

  71. [71]

    Tachikawa, On gauging finite subgroups , http://dx.doi.org/10.21468/SciPostPhys.8.1.015 SciPost Phys

    Y. Tachikawa, On gauging finite subgroups , http://dx.doi.org/10.21468/SciPostPhys.8.1.015 SciPost Phys. 8 (2020) 015 , http://arxiv.org/abs/1712.09542 arXiv:1712.09542 [hep-th]

  72. [72]

    Thorngren and Y

    R. Thorngren and Y. Wang, Fusion category symmetry. Part I. Anomaly in-flow and gapped phases , http://dx.doi.org/10.1007/JHEP04(2024)132 JHEP 04 (2024) 132 , http://arxiv.org/abs/1912.02817 arXiv:1912.02817 [hep-th]

  73. [73]

    Mapping topological to conformal field theories through strange correlators

    R. Vanhove, M. Bal, D. J. Williamson, N. Bultinck, J. Haegeman, and F. Verstraete, Mapping topological to conformal field theories through strange correlators , http://dx.doi.org/10.1103/PhysRevLett.121.177203 Phys. Rev. Lett. 121 (2018) 177203 , http://arxiv.org/abs/1801.05959 arXiv:1801.05959 [quant-ph]

  74. [74]

    Vancraeynest-De Cuiper, J

    B. Vancraeynest-De Cuiper, J. C. Bridgeman, N. Dewolf, J. Haegeman, and F. Verstraete, One-dimensional symmetric phases protected by frieze symmetries , http://dx.doi.org/10.1103/PhysRevB.107.115123 Phys. Rev. B 107 (2023) 115123 , http://arxiv.org/abs/2202.12880 arXiv:2202.12880 [cond-mat.str-el]

  75. [75]

    Vancraeynest-De Cuiper and C

    B. Vancraeynest-De Cuiper and C. Delcamp, Twisted gauging and topological sectors in (2+1)d Abelian lattice gauge theories , http://dx.doi.org/10.21468/SciPostPhys.19.2.054 SciPost Phys. 19 (2025) 054 , http://arxiv.org/abs/2501.16301 arXiv:2501.16301 [cond-mat.str-el]

  76. [76]

    Vancraeynest-De Cuiper and J

    B. Vancraeynest-De Cuiper and J. Garre-Rubio, Systematic construction of stabilizer codes via gauging abelian boundary symmetries , http://dx.doi.org/10.22331/q-2025-09-08-1852 Quantum 9 (2025) 1852 , http://arxiv.org/abs/2410.09044 arXiv:2410.09044 [quant-ph]

  77. [77]

    Vanhove, L

    R. Vanhove, L. Lootens, H.-H. Tu, and F. Verstraete, Topological aspects of the critical three-state Potts model , http://dx.doi.org/10.1088/1751-8121/ac68b1 J. Phys. A 55 (2022) 235002 , http://arxiv.org/abs/2107.11177 arXiv:2107.11177 [math-ph]

  78. [78]

    Vanhove, L

    R. Vanhove, L. Lootens, M. Van Damme, R. Wolf, T. J. Osborne, J. Haegeman, and F. Verstraete, Critical Lattice Model for a Haagerup Conformal Field Theory , http://dx.doi.org/10.1103/PhysRevLett.128.231602 Phys. Rev. Lett. 128 (2022) 231602 , http://arxiv.org/abs/2110.03532 arXiv:2110.03532 [cond-mat.stat-mech]

  79. [79]

    Verstraete, M

    F. Verstraete, M. M. Wolf, D. Perez-Garcia, and J. I. Cirac, Criticality, the area law, and the computational power of projected entangled pair states, Phys. Rev. Lett. 96 (2006) 220601 https://link.aps.org/doi/10.1103/PhysRevLett.96.220601

  80. [80]

    D. J. Williamson, N. Bultinck, M. Mari \"e n, M. B. S ahino g lu, J. Haegeman, and F. Verstraete, Matrix product operators for symmetry-protected topological phases: Gauging and edge theories , http://dx.doi.org/10.1103/PhysRevB.94.205150 Phys. Rev. B 94 (2016) 205150 , http://arxiv.org/abs/1412.5604 arXiv:1412.5604 [quant-ph]

Showing first 80 references.