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On gauging finite subgroups
by Yuji Tachikawa
This is not the latest submitted version.
Submission summary
| Authors (as registered SciPost users): | Yuji Tachikawa |
| Submission information | |
|---|---|
| Preprint Link: | https://arxiv.org/abs/1712.09542v2 (pdf) |
| Date submitted: | June 7, 2018, 2 a.m. |
| Submitted by: | Yuji Tachikawa |
| Submitted to: | SciPost Physics |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
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| Approach: | Theoretical |
Abstract
We study in general spacetime dimension the symmetry of the theory obtained by gauging a non-anomalous finite normal Abelian subgroup $A$ of a $\Gamma$-symmetric theory. Depending on how anomalous $\Gamma$ is, we find that the symmetry of the gauged theory can be i) a direct product of $G=\Gamma/A$ and a higher-form symmetry $\hat A$ with a mixed anomaly, where $\hat A$ is the Pontryagin dual of $A$; ii) an extension of the ordinary symmetry group $G$ by the higher-form symmetry $\hat A$; iii) or even more esoteric types of symmetries which are no longer groups. We also discuss the relations to the effect called the $H^3(G,\hat A)$ symmetry localization obstruction in the condensed-matter theory and to some of the constructions in the works of Kapustin-Thorngren and Wang-Wen-Witten.
Current status:
Reports on this Submission
Report #1 by Anonymous (Referee 1) on 2018-7-11 (Invited Report)
- Cite as: Anonymous, Report on arXiv:1712.09542v2, delivered 2018-07-11, doi: 10.21468/SciPost.Report.531
Strengths
- clearly written
- gives nice overview of important subject of generalized symmetry
- finds good balance between general theory and concrete examples
Weaknesses
Report
Requested changes
- Footnote 1: Why does the doubled coset appear as a label set for domain walls?
- Footnote 1: Does "consistent set of topological defects" mean that it is closed with respect to fusion?
- Page 3, Notations and conventions: Please give a brief reminder on "n-form symmetry". How does it relate to n-groupoids? (This is connected to item 14 below.)
- Page 3, Notations and conventions: At first I was confused by the dimensions of the spaces X and Y. Please briefly explain why the dimension D+1 appears even though spacetime is D-dimensional.
- Page 4, last paragraph: Its seems that this discussion is also a partial TFT interpretation of Pachner's theorem on D-dimensional triangulations. Has the author considered this in more detail?
- Page 6, boxed result: What exactly is Y here, and how does the result depend on it? Why was it not mentioned more prominently earlier in Section 2?
- Page 7: Why does gh in G serve as a source (and not as target) of the domain wall?
- Page 8: Please give more details for the last paragraph before Section 2.3.
- Footnote 5: I would have thought that the non-commutative algebra "defines" the space M indirectly, not directly.
- Page 9, last item: One could argue that the extension to a 3-functor from BG to the 3-category of certain fusion categories and their bimodule categories (as studied by Etingof, Nikshych and Ostrik) is even more relevant in TQFT; in this case there is also an H^4-obstruction.
- Page 14, second paragraph of Section 2.7: Please give a reference for the well-known result.
- Page 17, first paragraph of Section 3.3: In my copy of the paper Section 3.1 treats the case Z_n, not only Z_2.
- Page 18, last paragraph: What do the \otimes-symbols mean?
- Page 23: Is G_{[n]} really equal to B^nG?
- Typos:
- "Gaitto" on Page 2
- "two analysis" on Page 3
- "3)-chain" on Page 4
- "as also as" on Page 7
- "we know have" on Page 8
- "described blow" on Page 11
