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arxiv: 2312.16317 · v3 · submitted 2023-12-26 · ✦ hep-th · cond-mat.str-el· math.QA

Non-Invertible Anyon Condensation and Level-Rank Dualities

Pith reviewed 2026-05-24 05:37 UTC · model grok-4.3

classification ✦ hep-th cond-mat.str-elmath.QA
keywords non-invertible anyon condensationlevel-rank dualitytopological quantum field theoryChern-Simons theoryconformal embeddingsMaverick cosetsparafermion theoryrational conformal field theory
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The pith

Non-invertible anyon condensation generates generalized level-rank dualities for three-dimensional topological quantum field theories.

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

The paper shows that dualities between three-dimensional topological quantum field theories often rely on condensing non-invertible anyons, which are topological lines with non-group-like fusion rules. This approach generalizes the usual level-rank dualities of Chern-Simons theories and brings together disparate phenomena such as conformal embeddings and Maverick cosets in the boundary rational conformal field theories. The authors provide explicit constructions for infinite families of such dualities, including a new expression for the parafermion theory and alternative forms for certain c=1 conformal field theories and SU(2) theories at level N. A sympathetic reader would see this as a unifying mechanism that explains why certain exceptional cases appear in the classification of these theories.

Core claim

The authors derive that non-abelian anyon condensation, defined as the gauging of collections of topological lines with non-invertible fusion rules, produces new dualities that generalize level-rank dualities. This condensation unifies conformal embeddings and Maverick cosets, with examples including the parafermion theory as (SU(N)_2 × Spin(N)_{-4})/A_N, points on the c=1 orbifold as (Spin(2N)_2 × Spin(N)_{-2} × Spin(N)_{-2})/B_N, and SU(2)_N as (USp(2N)_1 × SO(N)_{-4})/C_N.

What carries the argument

non-abelian anyon condensation, the gauging of topological lines whose fusion rules are not those of a group

If this is right

  • The dualities hold for infinite series involving the quotients A_N, B_N, and C_N.
  • Exceptional phenomena in TQFTs and RCFTs receive a uniform explanation through this condensation.
  • New presentations of known theories become available, such as the parafermion and orbifold CFTs.
  • The modular data of the condensed theories match those of the dual descriptions.

Where Pith is reading between the lines

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

  • This mechanism may classify a larger set of dualities than previously recognized.
  • Computations of boundary states or correlation functions could be simplified using the new presentations.
  • Extensions to other gauge groups or higher-rank cases might yield further dualities.

Load-bearing premise

That non-abelian anyon condensation can be performed consistently in these theories without producing inconsistencies in the modular data or the associated conformal field theories.

What would settle it

A mismatch between the modular S-matrix or central charge computed from the condensed theory and that of the claimed dual theory would falsify the duality.

Figures

Figures reproduced from arXiv: 2312.16317 by Clay Cordova, Diego Garc\'ia-Sep\'ulveda.

Figure 1
Figure 1. Figure 1: On the left: the theory (Gk × H−k˜)/Z, where the common center Z of Gk and H−k˜ has been gauged, in the presence of the CFT coset boundary condition which is denoted (Gk/Hk˜)Z. On the right: a topological interface connecting the product Gk × H−k˜ without the common center gauged and (Gk × H−k˜)/Z. let us deduce why (2.4) is correct. In particular, we would like to understand the difference between the bou… view at source ↗
Figure 2
Figure 2. Figure 2: Coset boundary condition with single vacuum ( [PITH_FULL_IMAGE:figures/full_fig_p012_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Pushing the topological interface towards the boundary and fusing it with the coset bound [PITH_FULL_IMAGE:figures/full_fig_p012_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: In the canonical CFT boundary condition (in orange), all lines of the bulk CS theory end [PITH_FULL_IMAGE:figures/full_fig_p014_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: In a topological boundary condition not all lines of the bulk theory end perpendicularly [PITH_FULL_IMAGE:figures/full_fig_p015_5.png] view at source ↗
read the original abstract

We derive new dualities of topological quantum field theories in three spacetime dimensions that generalize the familiar level-rank dualities of Chern-Simons gauge theories. The key ingredient in these dualities is non-abelian anyon condensation, which is a gauging operation for topological lines with non-group-like i.e. non-invertible fusion rules. We find that, generically, dualities involve such non-invertible anyon condensation and that this unifies a variety of exceptional phenomena in topological field theories and their associated boundary rational conformal field theories, including conformal embeddings, and Maverick cosets (those where standard algorithms for constructing a coset model fail.) We illustrate our discussion in a variety of isolated examples as well as new infinite series of dualities involving non-abelian anyon condensation including: i) a new description of the parafermion theory as $(SU(N)_{2} \times Spin(N)_{-4})/\mathcal{A}_{N},$ ii) a new presentation of a series of points on the orbifold branch of $c=1$ conformal field theories as $(Spin(2N)_{2} \times Spin(N)_{-2} \times Spin(N)_{-2})/\mathcal{B}_{N}$, and iii) a new dual form of $SU(2)_{N}$ as $(USp(2N)_{1} \times SO(N)_{-4})/\mathcal{C}_{N}$ arising from conformal embeddings, where $\mathcal{A}_{N}, \mathcal{B}_{N},$ and $\mathcal{C}_{N}$ are appropriate collections of gauged non-invertible bosons.

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

2 major / 1 minor

Summary. The paper claims to derive new dualities of 3d TQFTs that generalize level-rank dualities of Chern-Simons theories. The key mechanism is non-abelian anyon condensation (gauging topological lines with non-group-like fusion rules). It asserts that this unifies exceptional phenomena including conformal embeddings and Maverick cosets, and provides explicit infinite families: the parafermion theory as (SU(N)_2 × Spin(N)_{-4})/A_N, c=1 orbifold points as (Spin(2N)_2 × Spin(N)_{-2} × Spin(N)_{-2})/B_N, and SU(2)_N as (USp(2N)_1 × SO(N)_{-4})/C_N, where A_N, B_N, C_N are collections of gauged non-invertible bosons.

Significance. If the non-invertible condensation constructions are shown to yield consistent TQFTs whose modular S/T matrices and central charges exactly reproduce the target theories for generic N, the result would unify a range of exceptional dualities and boundary phenomena under a single gauging operation, extending beyond abelian condensation.

major comments (2)
  1. [Abstract] Abstract: the claim that gauging the collections A_N, B_N, C_N produces consistent 3d TQFTs with matching modular data for the infinite families (parafermions, c=1 orbifolds, SU(2)_N) is load-bearing for the unification statement, yet the provided constructions do not include explicit verification that the resulting fusion rules remain anomaly-free and that the S-matrix and central charge reproduce the targets without post-hoc adjustments.
  2. [Abstract] Abstract: the assertion that 'generically, dualities involve such non-invertible anyon condensation' requires showing that the standard level-rank dualities emerge as special cases of the new construction or that the exceptional cases are covered without circular reliance on the target modular data to define the gauged lines.
minor comments (1)
  1. The definitions of the collections A_N, B_N, C_N are referred to only as 'appropriate collections'; explicit listing of the gauged lines and their fusion rules would improve readability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading and constructive feedback. We address the two major comments point by point below, proposing clarifications and additions where appropriate to strengthen the presentation of the infinite-family constructions.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the claim that gauging the collections A_N, B_N, C_N produces consistent 3d TQFTs with matching modular data for the infinite families (parafermions, c=1 orbifolds, SU(2)_N) is load-bearing for the unification statement, yet the provided constructions do not include explicit verification that the resulting fusion rules remain anomaly-free and that the S-matrix and central charge reproduce the targets without post-hoc adjustments.

    Authors: We agree that a more explicit verification for generic N would strengthen the unification claim. The manuscript defines the collections A_N, B_N, C_N from the fusion rules of the parent theories and verifies consistency (including anomaly-freeness via the condensation procedure and central-charge matching) for representative small N in the examples; the general case follows from the topological properties of non-invertible condensation. We will add an appendix with explicit S- and T-matrix computations for additional small N together with a general argument that the post-condensation fusion rules remain consistent without reference to the target data. revision: yes

  2. Referee: [Abstract] Abstract: the assertion that 'generically, dualities involve such non-invertible anyon condensation' requires showing that the standard level-rank dualities emerge as special cases of the new construction or that the exceptional cases are covered without circular reliance on the target modular data to define the gauged lines.

    Authors: Section 2 and the beginning of Section 4 show that ordinary level-rank dualities are recovered when the relevant anyons become invertible (e.g., at specific small values of N where the fusion rules reduce to group-like). The lines in A_N, B_N, C_N are identified directly from the fusion category of the parent TQFTs (SU(N)_2 × Spin(N)_{-4}, etc.) prior to any reference to the target modular data, so the construction is not circular. We will add a short clarifying paragraph emphasizing this independence. revision: partial

Circularity Check

0 steps flagged

Minor self-citation not load-bearing; central derivation independent

full rationale

The paper introduces non-invertible anyon condensation as a gauging operation on topological lines and applies it to construct explicit dualities such as (SU(N)_2 × Spin(N)_{-4})/A_N for parafermions. The derivation proceeds by defining the collections A_N, B_N, C_N and verifying the resulting modular data and central charges match target theories. No equation reduces a claimed prediction to a fitted input or self-referential definition. Prior self-citations supply background on non-invertible symmetries but do not bear the load of proving consistency or uniqueness for the new families; those rest on direct construction. The result is therefore self-contained against external modular-data benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 1 invented entities

The work rests on standard TQFT and fusion-category axioms while introducing new specific gauging collections for the examples; no obvious free parameters are fitted to data.

axioms (1)
  • domain assumption Three-dimensional TQFTs admit consistent gauging operations on topological lines whose fusion rules are non-invertible.
    Invoked as the key ingredient enabling the new dualities.
invented entities (1)
  • Collections A_N, B_N, C_N of gauged non-invertible bosons no independent evidence
    purpose: To define the specific anyon condensation operations that realize the dualities for parafermions, orbifold points, and SU(2)_N.
    Introduced in the abstract as the appropriate collections for each family of examples.

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Forward citations

Cited by 2 Pith papers

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  2. Homomorphism, substructure, and ideal: Elementary but rigorous aspects of renormalization group or hierarchical structure of topological orders

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