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Gapped Phases in (2+1)d with Non-Invertible Symmetries: Part II

by Lakshya Bhardwaj, Sakura Schafer-Nameki, Apoorv Tiwari, Alison Warman

Submission summary

Authors (as registered SciPost users): Apoorv Tiwari · Alison Warman
Submission information
Preprint Link: https://arxiv.org/abs/2502.20440v2  (pdf)
Date submitted: June 7, 2025, 12:25 a.m.
Submitted by: Apoorv Tiwari
Submitted to: SciPost Physics
Ontological classification
Academic field: Physics
Specialties:
  • Condensed Matter Physics - Theory
  • High-Energy Physics - Theory

Abstract

We use the Symmetry Topological Field Theory (SymTFT) to systematically characterize gapped phases in 2+1 dimensions with categorical symmetries. The SymTFTs that we consider are (3+1)d Dijkgraaf-Witten (DW) theories for finite groups $G$, whose gapped boundaries realize all so-called ``All Bosonic type" fusion 2-category symmetries. In arXiv:2408.05266 we provided the general framework and studied the case where $G$ is an abelian group. In this work we focus on the case of non-Abelian $G$. Gapped boundary conditions play a central role in the SymTFT construction of symmetric gapped phases. These fall into two broad families: minimal and non-minimal boundary conditions, respectively. The first kind corresponds to boundaries on which all line operators are obtainable as boundary projections of bulk line operators. The symmetries on such boundaries include (anomalous) 2-groups and 2-representation categories of 2-groups. Conversely non-minimal boundaries contain line operators that are intrinsic to the boundaries. The symmetries on such boundaries correspond to fusion 2-categories where modular tensor categories intertwine non-trivially with the above symmetry types. We discuss in detail the generalized charges of these symmetries and their condensation patterns that give rise to a zoo of rich beyond-Landau gapped phases. Among these are phases that exhibit novel patterns of symmetry breaking wherein the symmetry broken vacua carry distinct kinds of topological order. We exemplify this framework for the case where $G$ is a dihedral group.

Author indications on fulfilling journal expectations

  • Provide a novel and synergetic link between different research areas.
  • Open a new pathway in an existing or a new research direction, with clear potential for multi-pronged follow-up work
  • Detail a groundbreaking theoretical/experimental/computational discovery
  • Present a breakthrough on a previously-identified and long-standing research stumbling block
Current status:
Awaiting resubmission

Reports on this Submission

Report #2 by Anonymous (Referee 2) on 2025-7-28 (Invited Report)

Strengths

The "superstar" examples are of potential significance.

Weaknesses

  1. Methodology is a bit outdated. The mathmatical theory of fusion 2-categories has been intensely devoloped in recently years. However, this work did not embrace those developments and used simple-minded treatments, sometimes proceed by guessing or trial-and-error. The general framework presented in Section 2 is incomplete and inaccurate. A number of errors and inaccuracies can be found in the details of the examples.
  2. Organization is poor. The majority of the manuscript is devoted to technical details of S3 and D8 examples. This is also a sign that the authors lack confidence in their general theory. If the general framework and algorithm could be laid down clearly, the reader should be able to reproduce examples, and then only essential details of (important) examples need to be listed.
  3. Not clearly written. In particular, the design of conventions and notations is messy and difficult to follow. For example, in Table 2, the same object (BDir and 2VecS3) is given different names, which is technically unnecessary and only make things complicated. New symbols often appear without clear explanation.

Report

The manuscript needs substantial polishment before it can meet the publication criteria of SciPost Physics. Here are some potential suggestion: 1. Improve the section on the general framework, making it repeatable. 2. On the exmaples, focus on the interesting "superstar" examples, and reduce the amount the details on the well-known or less-interesting examples. 3. See also the requested changes.

Requested changes

  1. Under Table 1, the names all-boson, emergent-fermion, and the abbreviations AB and EF date back to the original papers [65] and its sequal Phys. Rev. X 9, 021005. [52] relies heavily on the idea of these two works but failed to address the credit. Appropriate citations should be added. Footnote 2 is questionable. EF-type fusion 2-categories are by definition fermionic fusion 2-categories. It is the Drinfeld centre (or SymTFT) of an EF-type fusion 2-category that is a bosonic 4d topological order. Compare, in 2d, sVec is a fermionic symmetry and Z(sVec) is the toric code.
  2. Below (2.18), "The relation to H-double cosets is due to the fact that the number of H-conjugacy classes into which a G-conjugacy class splits is equal to the number of double cosets HgH that intersect the G-conjugacy class." The statement should be more precise. Only saying "the number is equal" is pointless.
  3. Table 3, row 3: What is the two group $\mathbb G^{(2)}$ when $H$ is not normal and $G/H$ is not a group?
  4. Equation (2.32): What is the precise meaning of vacua? (It seems to mean idempotent local operators by later parts) How is this formula derived?
  5. Above equaiton (2.42), the notation ($G/H$-SSB)$\boxtimes$($H$-SPT) is misleading for a mixed SSB and SPT phase since it indicates a decoupled stacking.
  6. The term "topological local operators" looks self-contradictary; by definition topological means non-local. Here the notion of locality secretly changes upon compatification of the SymTFT: a topological operator in the 4d SymTFT becomes a local operator in the 3d theory after compatification. It may be better to use just local operator.
  7. Discussions around equation (2.46) are questionable. Where does the basis $|g\rangle$ come from? $D^R(g)$ is a matrix acting on $R$, shouldn't one choose basis from $R$? Otherwise how can (2.46) make sense?
  8. Various terminology and notions are used without clear explanations on their first occurrence: (un)twisted sectors, Triv in (3.55), $1_{00}$ in (3.67).
  9. Around (3.65) and (3.103): It is weird to "assume" how $L^{1,2}$ interacts with $v_0$. Shouldn't this be computable from their algebras? Can't the author compute $L^{1,2}v_0$ and $L^{1,2}v_1$? How can these be "indistinguishable" and require some additional assumption to proceed?
  10. (3.118), new symbol $\lambda$ does not come with an explanation.
  11. (3.147), wrong label on the physical boundary.
  12. Above (3.223), "Therefore each vacuum realizes a T topological order described by T = Z(C)." C needs explanation. Also, the authors keep distinguishing physical theories (boundary conditions) from their mathematical (categorical) descriptions, but here they ironically equate them.
  13. (4.33), the same graph on both sides.

Recommendation

Ask for major revision

  • validity: -
  • significance: -
  • originality: -
  • clarity: -
  • formatting: -
  • grammar: -

Report #1 by Anonymous (Referee 1) on 2025-7-27 (Invited Report)

Strengths

1- Interesting class of gapped phases, especially what the authors refer to as the "super-star" phase where a trivial and a topologically ordered phase coexist.

2-Several concrete and detailed examples.

Weaknesses

1-Too long, longer than Part I.

Report

This is a very nice series of works and I am curious to see where the authors take it from here. I may lack the math background required to appreciate this work completely, so there might be some mathematical inaccuracies that I am not aware of (I was looking through the reports of the previous two papers and noticed that the referees pointed out a few inaccuracies). But the explicit examples discussed in Sec. 3, 4, and 5 make it easy to follow the underlying physics, which seems on the mark to me.

This paper clearly meets the general acceptance criteria of SciPost Physics. It also uncovers several new and interesting gapped phases with non-invertible symmetries, so it does meet one of the expectations of SciPost Physics. However, I am not sure what makes it "provide a novel and synergetic link between different research areas".

Requested changes

1-There are several typos throughout the paper, both grammatical and mathematical. I urge the authors to proofread it thoroughly.

2-Perhaps this is my ignorance, but I am confused by the use of $\otimes$ vs $\boxtimes$ and $\oplus$ vs $\boxplus$. Could the authors explain the difference, at least in a footnote, when these notations are introduced for the first time? This could be, for example, around Table 2.

Recommendation

Publish (easily meets expectations and criteria for this Journal; among top 50%)

  • validity: high
  • significance: high
  • originality: good
  • clarity: good
  • formatting: excellent
  • grammar: excellent

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