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Superconformal index with surface defects for class ${\cal S}_k$
High Energy Physics - Theory · Submitted 6 Jun 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We compute the index of the 4d-2d systems and reproduce the results obtained from the first method.
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The abstract, sentence by sentence
We study surface defects in 4d $\mathcal{N}=1$ $SU(N)$ superconformal gauge theories of class $\mathcal{S}_k$ obtained from the 6d (1,0) theories of type $A_{N-1}$, which are worldvolume theories on $N$ M5-branes at $\mathbb{C}^2/\mathbb{Z}_k$ singularities, compactified on Riemann surfaces with punctures. First we apply a method based on Riemann surface description and obtain the superconformal index of the theories in the presence of surface defects labelled by arbitrary symmetric representations of $su(N)$. Then we propose another description for the same surface defects, which involves 4d-2d coupled systems, by identifying which 2d $\mathcal{N}=(0,2)$ theories should be coupled. We compute the index of the 4d-2d systems and reproduce the results obtained from the first method. Finally we study the 2d TQFT structure of the index for class $\mathcal{S}_{k}$ theories by obtaining several eigenfunctions and eigenvalues of the difference operators that capture the surface defects and checking their relation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study surface defects in 4d $\mathcal{N}=1$ $SU(N)$ superconformal gauge theories of class $\mathcal{S}_k$ obtained from the 6d (1,0) theories of type $A_{N-1}$, which are worldvolume theories on $N$ M5-branes at $\mathbb{C}^2/\mathbb{Z}_k$ singularities, compactified on Riemann surfaces with punctures. | background 0.54 | 0.31 | 0.05 | asserted 0.98 |
| s1 | First we apply a method based on Riemann surface description and obtain the superconformal index of the theories in the presence of surface defects labelled by arbitrary symmetric representations of $su(N)$. | method 0.63 | 0.95 | 0.12 | asserted 1.00 |
| s2 | Then we propose another description for the same surface defects, which involves 4d-2d coupled systems, by identifying which 2d $\mathcal{N}=(0,2)$ theories should be coupled. | method 0.72 | 0.90 | 0.09 | asserted 0.88 |
| s3 | We compute the index of the 4d-2d systems and reproduce the results obtained from the first method. | result 0.84 | 0.95 | 0.22 | asserted 1.00 |
| s4 | Finally we study the 2d TQFT structure of the index for class $\mathcal{S}_{k}$ theories by obtaining several eigenfunctions and eigenvalues of the difference operators that capture the surface defects and checking their relation. | contribution 0.89 | 0.95 | 0.24 | asserted 1.00 |
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The paper
Original abstract
We study surface defects in 4d $\mathcal{N}=1$ $SU(N)$ superconformal gauge theories of class $\mathcal{S}_k$ obtained from the 6d (1,0) theories of type $A_{N-1}$, which are worldvolume theories on $N$ M5-branes at $\mathbb{C}^2/\mathbb{Z}_k$ singularities, compactified on Riemann surfaces with punctures. First we apply a method based on Riemann surface description and obtain the superconformal index of the theories in the presence of surface defects labelled by arbitrary symmetric representations of $su(N)$. Then we propose another description for the same surface defects, which involves 4d-2d coupled systems, by identifying which 2d $\mathcal{N}=(0,2)$ theories should be coupled. We compute the index of the 4d-2d systems and reproduce the results obtained from the first method. Finally we study the 2d TQFT structure of the index for class $\mathcal{S}_{k}$ theories by obtaining several eigenfunctions and eigenvalues of the difference operators that capture the surface defects and checking their relation.
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References
How the literature uses it
16 arXiv papers cite this in 22 sentences
Papers citing it · 16 sentences without a confident label
Builds on it 1 paper
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Building on [ref], a surface defect of type $(r,s)$ can be introduced via a position dependent VEV [ref] which is related to a pole at
Elliptic Quantum Curves of Class $\mathcal{S}_k$ · Higgsing to defects · 0.92
Uses its method or tool 1 paper
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In [ref] , a prescription to evaluate the Schur index in the presence of a class of surface operators was proposed, which we call the “Higgsing prescription.”[See [ref] for earlier applications of this prescription.]
On the Correspondence between Surface Operators in Argyres-Douglas Theories and Modules of Chiral Algebra · Higgsing prescription · 0.91
Compares with it 1 paper
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For $N > 2$, the transfer matrix is consistent with the result found in [ref] , where the action of surface defects in the symmetric powers of the vector representation was computed for restricted values of the spectral parameters.
Surface defects and elliptic quantum groups · $= 1$ supersymmetric quiver gauge theories and surface defects · 0.97
Cites it as background 3 papers
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The full characteristics of the surface operator as the disorder one is less understood than those of the order operator like a Wilson line, though lots of attempts to completely classify the surface operator have been archived (e.g., see [ref] and a comprehensive review [ref] ).
Surface Operators from M-strings · Introduction and summary · 1.00
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Examples of $(0,2)$ surface defects, though mostly in 4d theories, can be found in the literature [ref] , see also [ref] via breaking of $(2,2)$ defects, and [ref] for variety of other $(2,2)$ and $(4,4)$ examples, including [ref] where a $(4,4)$ surface defect is broken down to $(0,2)$ by the fugacities.
Interfaces and Quantum Algebras, II: Cigar Partition Function · Supersymmetric observables · 0.97
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For example integrable systems derived using compactifications of the worldvolume theory of $k$ M5 branes probing $A_N-1$ singularity were shown to be related to the set of transfer matrices [ref] .
$C_2$ generalization of the van Diejen model from the minimal $(D_5,D_5)$ conformal matter · Discussion and outlook. · 0.88
What it cites · 29 sentences without a confident label
Builds on 1 paper
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With the help of the expressions for $A_1$ case in [ref] , we expect that the normalized functions $_$ are orthogonal under the following measure $$ for $A_N-1$ case [equation] where the q-Pochhammer symbol $(x;q)$ is defined as ([ref]).
N=1 theories of class S_k · TQFT structure · 0.86
Uses the method or tool of 3 papers
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In order to capture the surface defects, the authors in [ref] introduced the following procedure.
N=1 theories of class S_k · Surface defects from Riemann surface description · 0.84
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The elliptic genus [ref] of this model is written as ℐ_ell(ζ^(i)_a, ζ̃^(i)_a,c,d,t;q) = 1/|W|∑_ω_* JK `-Res (𝐐(ω_*), η) Z_1`- loop .
Elliptic genera of two-dimensional N=2 gauge theories with rank-one gauge groups · 2d $𝒩=(0,2)$ elliptic genus and 4d-2d coupled system for surface defect · 0.95
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The elliptic genus [ref] of this model is written as ℐ_ell(ζ^(i)_a, ζ̃^(i)_a,c,d,t;q) = 1/|W|∑_ω_* JK `-Res (𝐐(ω_*), η) Z_1`- loop .
Elliptic genera of 2d N=2 gauge theories · 2d $𝒩=(0,2)$ elliptic genus and 4d-2d coupled system for surface defect · 0.95
Compares with 1 paper
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We evaluated the elliptic genus of these two classes of two dimensional $𝒩=(0,2)$ gauge theories and found that the 4d-2d combined index reproduces the superconformal indiex with surface defects obtained as in [ref] up to the overall fractional fugacity shift.
N=1 theories of class S_k · Conclusion · 1.00
Cites as background 8 papers
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First we review class $_k$ theories, which are certain 4d $=1$ SCFTs and were associated to Riemann surfaces in [ref] .
N=1 theories of class S_k · Class $_k$ theories · 1.00
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Inspired by the relation between the 4d SCFTs and the Riemann surfaces, the authors of [ref] and [ref] introduced a systematic formalism that computes superconformal index of these 4d SCFTs in terms of the Riemann surface description.
S-duality and 2d Topological QFT · Introduction · 0.86
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Inspired by the relation between the 4d SCFTs and the Riemann surfaces, the authors of [ref] and [ref] introduced a systematic formalism that computes superconformal index of these 4d SCFTs in terms of the Riemann surface description.
The 4d Superconformal Index from q-deformed 2d Yang-Mills · Introduction · 0.86
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