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Supersymmetric Ground States of 3d $\mathcal{N}=4$ Gauge Theories on a Riemann Surface
by Mathew Bullimore, Andrea Ferrari, Heeyeon Kim
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Authors (as registered SciPost users):  Andrea Ferrari · Heeyeon Kim 
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Preprint Link:  https://arxiv.org/abs/2105.08783v2 (pdf) 
Date submitted:  20210906 15:22 
Submitted by:  Kim, Heeyeon 
Submitted to:  SciPost Physics 
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Academic field:  Physics 
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Approach:  Theoretical 
Abstract
This paper studies supersymmetric ground states of 3d $\mathcal{N}=4$ supersymmetric gauge theories on a Riemann surface of genus $g$. There are two distinct spaces of supersymmetric ground states arising from the $A$ and $B$ type twists on the Riemann surface, which lead to effective supersymmetric quantum mechanics with four supercharges and supermultiplets of type $\mathcal{N}=(2,2)$ and $\mathcal{N}=(0,4)$ respectively. We compute the space of supersymmetric ground states in each case, graded by flavour and Rsymmetries and in different chambers for real mass and FI parameters, for a large class of supersymmetric gauge theories. The results are formulated geometrically in terms of the Higgs branch geometry. We perform extensive checks of compatibility with the twisted index and mirror symmetry.
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Anonymous Report 2 on 2021111 (Invited Report)
 Cite as: Anonymous, Report on arXiv:2105.08783v2, delivered 20211101, doi: 10.21468/SciPost.Report.3773
Report
The study of 3d $N=4$ theories has been one of the recent focal points of the interaction between physics and mathematics. In the manuscript, the authors study spaces of supersymmetric ground states of certain class of 3d $N=4$ gauge theories on a Riemann surface, with partial A or Btwist, and give them precise geometric interpretations. The result is interesting and novel, and I find the exposition systematic and detailed with many worked out examples. I believe the manuscript has surpassed the expectation and criteria for this journal and recommend it for publication.
I would like to entertain below a few ideas for further improving the manuscript:
 I find the Introduction to be a good summary of the content of the paper. However, as the assumptions on the Coulomb and the Higgs branches in the A and Btwist cases respectively are important parts of the scientific results of this work, maybe it a good idea to not ``bury the lead'' but instead make these assumptions more visible by including them in the Introduction.
 It might worth clarifying what the precise meaning of ``finitedimensional $N = 4$ supersymmetric quantum mechanics'' is in the second paragraph of Section 1.1. With finitedimensional target, the full Hilbert space of the SQM can be still infinite dimensional.
 On the same page, the condition that $d$ is larger than $g$ seems only make sense for $U(1)$ subgroups of $G$.
 The authors find the Berry connection in the space of parameters is flat. Since this space can be nonsimplyconnected due to values of parameters that close the gap in the SQM spectrum, there is still the possibility of having nontrivial monodromies. It might be interesting for the author to comment on whether (or when) they exist.
 The mirror symmetry at the level of SQM ground states is a very interesting subject. However, the only example given in Section 8 is selfmirror. It might be a good idea to include another example with a more nontrivial mirror pair.
Anonymous Report 1 on 20211028 (Invited Report)
 Cite as: Anonymous, Report on arXiv:2105.08783v2, delivered 20211028, doi: 10.21468/SciPost.Report.3752
Report
I think the paper easily meets the acceptance criteria for this journal and
I recommend its publication. However, I have a few questions/comments (listed in the report) that I would like the authors to address, prior to publication.
Author: Heeyeon Kim on 20211119 [id 1961]
(in reply to Report 1 on 20211028)
The authors would like to thank the referee for the comments and suggestions.

In eq. (5.9), we consider a nontrivial background flux for the $U(1)$ flavor symmetry that corresponds to the line bundle $L$ with degree $d$ in eq. (5.1). On the other hand, for simplicity, we turn off the flux for the $U(1)$ topological symmetry in section 7.2. Mirror symmetry would work for all $d$ once we consider nontrivial backgrounds for the topological symmetry in the Btwist.

The large mass limit is indeed a computational trick in the Btwist and is not related to the large $\widetilde \zeta$ limit in the Atwist. The mass parameter is dual to $\zeta$, which is held fixed in a given chamber. Taking a large mass limit does not change the result as long as we stay in a chamber in the space of real mass parameters.

We expect that the mirror symmetry holds in the limit $e^2\rightarrow \infty, \zeta\rightarrow 0$. However, in this limit, noncompact directions emerge in the field space, which renders the space of supersymmetric ground states illdefined.

Reference added on page 20, typos corrected.
Author: Heeyeon Kim on 20211119 [id 1962]
(in reply to Report 2 on 20211101)The authors would like to thank the referee for the comments and suggestions.
We added a paragraph on the first page stating our assumptions.
In response to comments 2 and 3, we changed the corresponding sentences in the second paragraph and in the beginning of the fourth paragraph in section 1.1.
Singularities are real codimension one hyperplanes in the space of real mass parameters and therefore there's no notion of monodromy for the Berry connections.
The mirror symmetry is shown for the general abelian quivers in appendix B. It is straightforward to combine the analysis of SQCD discussed in detail in the main body of the paper to understand more nontrivial mirror examples.