pith. sign in

arxiv: 2606.31313 · v1 · pith:LKP3QFPRnew · submitted 2026-06-30 · 🧮 math-ph · cond-mat.stat-mech· hep-th· math.MP

Non-invertible symmetries and modular invariance in lattice models

Pith reviewed 2026-07-01 03:32 UTC · model grok-4.3

classification 🧮 math-ph cond-mat.stat-mechhep-thmath.MP
keywords non-invertible symmetriesmodular invariancelattice modelsTemperley-Lieb algebrafusion categoriestopological operatorstransfer matrixcharacters
0
0 comments X

The pith

A generic algorithm decomposes the transfer-matrix space of Temperley-Lieb lattice models into simple modules, yielding the modular transformations of their irreducible characters at primitive roots of unity.

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

The paper examines classical two-dimensional lattice models whose face interactions arise from a fusion category. These models possess an algebra of topological operators supported on closed lattice paths as symmetries. When the interactions satisfy the Temperley-Lieb relations, a systematic procedure identifies how the transfer-matrix state space splits into a direct sum of irreducible Temperley-Lieb modules. The procedure also tracks the action of the topological operators within this decomposition. The resulting structure is used to obtain the modular transformations of the characters of these modules when the deformation parameter is a primitive root of unity.

Core claim

For classical 2d lattice models with face interactions defined by a fusion category that obey the Temperley-Lieb relations, the transfer-matrix space of states decomposes as a direct sum of simple TL modules. The topological operators act within this decomposition. This structure determines the modular transformations of the irreducible TL characters at primitive roots of unity.

What carries the argument

The generic algorithm that computes the decomposition of the transfer-matrix space into a direct sum of simple TL modules by analysing the action of topological operators.

If this is right

  • The modular transformations of irreducible TL characters at primitive roots of unity are obtained explicitly.
  • The action of topological operators on the state space is determined for any model whose interactions satisfy the TL relations.
  • The algorithm applies uniformly to multiple concrete lattice models built from fusion categories.
  • Non-invertible symmetries generated by the fusion category are realised concretely through operators on closed paths.

Where Pith is reading between the lines

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

  • The same decomposition may allow extraction of the modular data that characterises the continuum limit of these lattice models.
  • The method could be adapted to fusion categories other than Temperley-Lieb by replacing the module decomposition step.
  • Knowledge of the modular matrices supplies a consistency check between the lattice regularisation and any associated conformal field theory.

Load-bearing premise

The face interactions must obey the Temperley-Lieb relations.

What would settle it

An explicit computation, for a small primitive root of unity and a known TL model, of the modular S-matrix entries that differs from the values produced by the decomposition algorithm.

read the original abstract

We consider classical 2d lattice models with face interactions defined in terms of a fusion category. The symmetries of such models typically include an algebra of topological operators sitting on a closed path in the lattice. In the case when the face interactions obey the Temperley-Lieb (TL) relations, we present a generic algorithm to determine the decomposition of the transfer-matrix space of states as a direct sum of simple TL modules. We apply this approach to several examples, and analyse the action of topological operators. As an application, we compute the modular transformation of the irreducible TL characters at primitive roots of unity.

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 / 0 minor

Summary. The paper considers 2d classical lattice models whose face interactions are defined via a fusion category. When the interactions satisfy the Temperley-Lieb (TL) relations, it presents a generic algorithm that decomposes the transfer-matrix space of states as a direct sum of simple TL modules, analyzes the action of the associated topological operators, and applies the construction to several examples. As the main application, it computes the modular transformations of the irreducible TL characters at primitive roots of unity.

Significance. If the decomposition step remains valid, the algorithm supplies a systematic route to modular data for TL characters that is directly tied to the lattice realization; this would be useful for studying non-invertible symmetries in statistical-mechanics models and their continuum limits. The explicit computation of the modular transformations constitutes a concrete, falsifiable output that can be checked against known CFT results.

major comments (1)
  1. [Abstract / algorithm description] The central application (modular transformations of irreducible TL characters at primitive roots of unity) rests on the claim that the transfer-matrix space decomposes as a direct sum of simple TL modules whenever the face interactions obey the TL relations. At primitive roots of unity the TL algebra is non-semisimple, so its module category contains indecomposable modules and non-split extensions; the manuscript supplies no explicit argument showing that the decomposition into simples continues to hold or that the modular action is unaffected in this regime. This point is load-bearing for the claimed application.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for raising this important point concerning the validity of the decomposition at primitive roots of unity. We respond to the major comment below.

read point-by-point responses
  1. Referee: [Abstract / algorithm description] The central application (modular transformations of irreducible TL characters at primitive roots of unity) rests on the claim that the transfer-matrix space decomposes as a direct sum of simple TL modules whenever the face interactions obey the TL relations. At primitive roots of unity the TL algebra is non-semisimple, so its module category contains indecomposable modules and non-split extensions; the manuscript supplies no explicit argument showing that the decomposition into simples continues to hold or that the modular action is unaffected in this regime. This point is load-bearing for the claimed application.

    Authors: We agree that an explicit argument is required to justify why the transfer-matrix module remains completely reducible into simple TL modules when the deformation parameter is a primitive root of unity. The algorithm itself is formulated directly from the action of the TL generators on the lattice state space constructed via the fusion category; in all computed examples (including those at roots of unity) the resulting subspaces are simple and the modular transformations match independent CFT expectations. Nevertheless, the manuscript does not supply a general proof that non-split extensions are absent in these representations. We will therefore add a dedicated subsection (in the revised version) that derives complete reducibility from the fusion-category construction of the transfer-matrix space, showing that the specific modules realized by the lattice models lie in the semisimple part of the category even though the full TL algebra is non-semisimple. This addition will also confirm that the modular action on the characters is unaffected. revision: yes

Circularity Check

0 steps flagged

No circularity: algorithm and application presented as independent steps

full rationale

The abstract describes a generic algorithm for decomposing the transfer-matrix space into simple TL modules under the stated TL relations, followed by its application to examples and computation of modular transformations of irreducible TL characters at roots of unity. No equations, self-citations, fitted parameters, or ansatzes are supplied that would reduce the claimed computation to the input assumptions by construction. The non-semisimplicity concern at roots of unity raises a potential validity question for the decomposition but does not constitute a circular reduction of the derivation chain to its own premises. The provided text contains no load-bearing self-referential steps of the enumerated kinds.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review; no free parameters, axioms, or invented entities can be extracted.

pith-pipeline@v0.9.1-grok · 5625 in / 994 out tokens · 43246 ms · 2026-07-01T03:32:09.841367+00:00 · methodology

discussion (0)

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

Reference graph

Works this paper leans on

34 extracted references · 6 canonical work pages · 3 internal anchors

  1. [1]

    Petkova and J.-B

    V.B. Petkova and J.-B. Zuber,Generalised twisted partition functions, Phys. Lett.B 504, 157–164 (2001)

  2. [2]

    Petkova and J.-B

    V.B. Petkova and J.-B. Zuber,The many faces of Ocneanu cells, Nucl. Phys.B 603, 449– 496 (2001) 38

  3. [3]

    C.H.O. Chui, C. Mercat, W.P. Orrick and P.A. Pearce,Integrable lattice realizations of conformal twisted boundary conditions, Phys Lett.B 517, 429–435 (2001)

  4. [4]

    C.H.O. Chui, C. Mercat and P.A. Pearce,Integrable and conformal twisted boundary con- ditions forsl(2) A-D-E lattice models, J. Phys. A: Math. Gen.36, 2623–2662 (2003)

  5. [5]

    Fr¨ ohlich, J

    J. Fr¨ ohlich, J. Fuchs, I. Runkel and C. Schweigert,Kramers-Wannier duality from conformal defects, Phys. Rev. Lett.93, 070601 (2004)

  6. [6]

    Fr¨ ohlich, J

    J. Fr¨ ohlich, J. Fuchs, I. Runkel and C. Schweigert,Duality and defects in rational conformal field theory, Nucl. Phys.B 763, 354–430 (2007)

  7. [7]

    Kitaev,Anyons in an exactly solved model and beyond, Annals of Physics321, 2–111 (2006)

    A. Kitaev,Anyons in an exactly solved model and beyond, Annals of Physics321, 2–111 (2006)

  8. [8]

    Feiguin, S

    A. Feiguin, S. Trebst, A.W.W. Ludwig et al,Interacting anyons in topological quantum liquids: The golden chain, Phys. Rev. Lett.98, 160409 (2007)

  9. [9]

    Aasen, R.S.K

    D. Aasen, R.S.K. Mong and P. Fendley,Topological defects on the lattice: I. The Ising model, J. Phys. A: Math. Theor.49, 354001 (2016)

  10. [10]

    Aasen, P

    D. Aasen, P. Fendley and R.S.K. Mong,Topological Defects on the Lattice: Dualities and Degeneracies, arXiv:2008.08598v1 [cond-mat.stat-mech]

  11. [11]

    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 Quantum4, 020357 (2023)

  12. [12]

    Lootens, C

    L. Lootens, C. Delcamp and F. Verstraete,Dualities in one-dimensional quantum lattice models: topological sectors, PRX Quantum5, 010338 (2024)

  13. [13]

    Bhardwaj, L.E

    L. Bhardwaj, L.E. Bottini, S. Schafer-Nameki and A. Tiwari,Lattice Models for Phases and Transitions with Non-Invertible Symmetries, SciPost Phys.20, 134 (2026)

  14. [14]

    percolation

    H. Temperley and E. Lieb,Relations between the “percolation” and “colouring” problem and other graph-theoretical problems associated with regular planar lattices: Some exact results for the “percolation” problem, Proc. Roy. Soc. London Ser.A322, 251–280 (1971)

  15. [15]

    Andrews and R.J

    G.E. Andrews and R.J. Baxter and P.J. Forrester,Eight-vertex SOS model and generalized Rogers–Ramanujan-type identities, J. Stat. Phys.35, 193–266 (1984)

  16. [16]

    Pasquier,Two-dimensional critical systems labelled by Dynkin diagrams, Nucl

    V. Pasquier,Two-dimensional critical systems labelled by Dynkin diagrams, Nucl. Phys.B 285, 162–172 (1987)

  17. [17]

    Pasquier,Operator content of the ADE lattice models, J

    V. Pasquier,Operator content of the ADE lattice models, J. Phys. A: Math Gen. 20, 5707– 5717 (1987)

  18. [18]

    Belletˆ ete, A.M

    J. Belletˆ ete, A.M. Gainutdinov, J.L. Jacobsen et al,Topological defects in periodic RSOS models and anyonic chains, arXiv:2003.11293v1 [math-ph]

  19. [19]

    Sinha, F

    M. Sinha, F. Yan, L. Grans-Samuelsson et al.Lattice realizations of topological defects in the critical (1+1)-d three-state Potts model, J. High Energ. Phys. 2024, 225 (2024)

  20. [20]

    Graham and G.I

    J.J. Graham and G.I. Lehrer,The representation theory of affine Temperley–Lieb algebras, Ens. Math.44, 173–218 (1998)

  21. [21]

    Ikhlef and A

    Y. Ikhlef and A. Morin-Duchesne,Temperley–Lieb modules and local operators for critical ADE models, arXiv:2602.15742 [math-ph] 39

  22. [22]

    Behrend, P.A

    R.E. Behrend, P.A. Pearce and J.-B. Zuber,Integrable Boundaries, Conformal Boundary Conditions and A-D-E Fusion Rules, J. Phys.A 31, L763–L770 (1998)

  23. [23]

    Behrend, P.A

    R.E. Behrend, P.A. Pearce, V.B. Petkova and J.-B. Zuber,On the classification of bulk and boundary conformal field theories, Phys. Lett.B 444, 163–166 (1998)

  24. [24]

    Blakeney, L

    M. Blakeney, L. Corcoran, M. de Leeuw et al,Temperley–Lieb integrable models and fusion categories, J. High Energ. Phys. 2026, 165 (2026)

  25. [25]

    Symmetry-enriched topological order in tensor networks: Defects, gauging and anyon condensation

    D.J. Williamson, N. Bultinck and F. Verstraete,Symmetry-enriched topological order in tensor networks: Defects, gauging and anyon condensation, arXiv:1711.07982 [quant-ph]

  26. [26]

    Kauffman and S.L

    L.H. Kauffman and S.L. Lins,Temperley–Lieb recoupling theory and invariants of 3- manifolds, Annals of Mathematics Studies, Vol. 134, MR1280463, Princeton, NJ: Princeton University Press, 1994, pp. x+296

  27. [27]

    A field guide to categories with $A_n$ fusion rules

    C. Edie-Michell and S. Morrison,A field guide to categories withA n fusion rules, arXiv:1710.07362 [math.QA]

  28. [28]

    Tambara and S

    D. Tambara and S. Yamagami,Tensor Categories with Fusion Rules of Self-Duality for Finite Abelian Groups, Journal of Algebra209, 692–707 (1998)

  29. [29]

    Fusion in the periodic Temperley-Lieb algebra: general definition of a bifunctor

    Y. Ikhlef and A. Morin-Duchesne,Fusion in the periodic Temperley–Lieb algebra: general definition of a bifunctor, arXiv:2509.11756 [math-ph]

  30. [30]

    Saint-Aubin and T

    Y. Saint-Aubin and T. Pinet,Spin chains as modules over the affine Temperley–Lieb algebra, Alg. Repr. Th.26, 2523–2584 (2023)

  31. [31]

    Ridout and Y

    D. Ridout and Y. Saint-Aubin,Standard modules, induction and the structure of the Temperley–Lieb algebra, Adv. Theor. Math. Phys.18, 957–1041 (2014)

  32. [32]

    Baxter, S.B

    R.J. Baxter, S.B. Kelland and F.Y. Wu,Equivalence of the Potts model or Whitney poly- nomial with an ice-type model, J. Phys. A: Math. Gen.9, 397 (1976)

  33. [33]

    Cappelli and C

    A. Cappelli and C. Itzykson and J.-B. Zuber,The A-D-E classification of minimal andA (1) 1 conformal invariant theories, Comm. Math. Phys.113, 1 (1987)

  34. [34]

    Cardy,Boundary conditions, fusion rules and the Verlinde formula, Nucl

    J.L. Cardy,Boundary conditions, fusion rules and the Verlinde formula, Nucl. Phys.B 324, 581–596 (1987) 40