SciPost Submission Page
On gauging finite subgroups
by Yuji Tachikawa
 Published as SciPost Phys. 8, 015 (2020)
Submission summary
As Contributors:  Yuji Tachikawa 
Arxiv Link:  https://arxiv.org/abs/1712.09542v3 (pdf) 
Date accepted:  20200109 
Date submitted:  20191224 01:00 
Submitted by:  Tachikawa, Yuji 
Submitted to:  SciPost Physics 
Academic field:  Physics 
Specialties: 

Approach:  Theoretical 
Abstract
We study in general spacetime dimension the symmetry of the theory obtained by gauging a nonanomalous 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 higherform 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 higherform 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 condensedmatter theory and to some of the constructions in the works of KapustinThorngren and WangWenWitten.
Ontology / Topics
See full Ontology or Topics database.Published as SciPost Phys. 8, 015 (2020)
Author comments upon resubmission
I summarized below the changes made according to the suggestions by the referee.
List of changes
1,2: A reference was added.
3: I added the information that an $n$form symmetry comes with a map to $K(G,n+1)$.
4: This is due to the fact that the general yoga says that the anomaly of a $D$dimensional theory is captured by a $(D+1)$dimensional invertible topological phase. I added a few references on this point. A short paragraph was added just before "organization of the note" to mention this important fact.
5: This was studied in the past; two references were added. I also explicitly mentioned which of the spacetimes $X_D$ and $Y_{D+1}$ were considered in various steps involved.
6: Indeed I should have mentioned the role of $Y$ more prominently. This I think is covered by the added paragraph mentioned in the point 4 above, and the clarification mentioned in the point 5 above.
7: The word "source" was used in the sense of the "source of (electric and other) charges" used in physics, and not in the sense of the source and the target. The word is changed to the "boundary", which more accurately captures the situation and should cause less confusion.
8: I tried to clarify the explanation by adding a few sentences describing an additional intermediate step, so that the original Figures 3,4,5 were replaced by the new Figures 3,4,5,6.
9: I agree with the referee's comment. I tried to clarify the footnote.
10: I agree with the referee's comment. A paragraph and two references were added.
11: The original article by Eilenberg and Mac Lane was added.
12: It was a carryover from an earlier version of the note; I thank the referee for the careful reading. They are corrected.
13: They are tensor product as $\mathbb{Z}$modules. This fact was made explicit.
14: Essentially, yes, but I would like to keep the notation $G_{[n]}$ as a shorthand for the (ordinary) group $G$ regarded as an $n$form symmetry.
15: I'd like to thank again the referee for the careful reading. They are all corrected.