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Argyres-Douglas Theories, Modularity of Minimal Models and Refined Chern-Simons
High Energy Physics - Theory · Submitted 25 Jan 2018
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The connection is made precise by showing how the modular transformation matrices of refined Chern-Simons theory are related to the proposed generalized ones for minimal models and the identification of Coulomb branch indices with the partition function of the refined Chern-Simons theory.
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The abstract, sentence by sentence
The Coulomb branch indices of Argyres-Douglas theories on $L(k,1)\times S^{1}$ are recently identified with matrix elements of modular transforms of certain $2d$ vertex operator algebras in a particular limit. A one parameter generalization of the modular transformation matrices of $(2N+3,2)$ minimal models are proposed to compute the full Coulomb branch index of $(A_{1},A_{2N})$ Argyres-Douglas theories on the same space. Morever, M-theory construction of these theories suggests direct connection to the refined Chern-Simons theory. The connection is made precise by showing how the modular transformation matrices of refined Chern-Simons theory are related to the proposed generalized ones for minimal models and the identification of Coulomb branch indices with the partition function of the refined Chern-Simons theory.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The Coulomb branch indices of Argyres-Douglas theories on $L(k,1)\times S^{1}$ are recently identified with matrix elements of modular transforms of certain $2d$ vertex operator algebras in a particular limit. | background 1.00 | 0.10 | 0.12 | asserted 1.00 |
| s1 | A one parameter generalization of the modular transformation matrices of $(2N+3,2)$ minimal models are proposed to compute the full Coulomb branch index of $(A_{1},A_{2N})$ Argyres-Douglas theories on the same space. | contribution 0.86 | 0.86 | 0.37 | asserted 0.53 |
| s2 | Morever, M-theory construction of these theories suggests direct connection to the refined Chern-Simons theory. | interpretation 0.55 | 0.20 | 0.08 | hedged possibility 1.00 |
| s3 | The connection is made precise by showing how the modular transformation matrices of refined Chern-Simons theory are related to the proposed generalized ones for minimal models and the identification of Coulomb branch indices with the partition function of the refined Chern-Simons theory. | result 0.53 | 0.87 | 0.70 | asserted 1.00 |
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Original abstract
The Coulomb branch indices of Argyres-Douglas theories on $L(k,1)\times S^{1}$ are recently identified with matrix elements of modular transforms of certain $2d$ vertex operator algebras in a particular limit. A one parameter generalization of the modular transformation matrices of $(2N+3,2)$ minimal models are proposed to compute the full Coulomb branch index of $(A_{1},A_{2N})$ Argyres-Douglas theories on the same space. Morever, M-theory construction of these theories suggests direct connection to the refined Chern-Simons theory. The connection is made precise by showing how the modular transformation matrices of refined Chern-Simons theory are related to the proposed generalized ones for minimal models and the identification of Coulomb branch indices with the partition function of the refined Chern-Simons theory.
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References
How the literature uses it
12 arXiv papers cite this in 18 sentences
Papers citing it · 16 sentences without a confident label
Compares with it 1 paper
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A one-parameter family of $S$ and $T$ matrices is also constructed in [ref] , which is related to our $S()$ and $T()$ by overall factors.
3d TQFTs from Argyres-Douglas theories · $(A_1, A_2)$ theory · 1.00
Cites it as background 1 paper
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Various interesting properties of 4d theory using 2d VOA are studied in [ref] .
W algebra, Cosets and VOA for 4d N = 2 SCFT from M5 branes · Known results · 0.98
What it cites · 48 sentences without a confident label
Builds on 1 paper
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We conjecture that Coulomb branch indices of $(A_1, A_2N)$ AD theories on lens space $L(k,1)$ times a circle can be written as (up to a proportional constant), [equation] where $_(A_1, A_2N)()$ and $_(A_1, A_2N)()$ are matrices with one parameter $$ which satisfies the following relations, [equation] Clearly $_(A_1, A_2N)()$ and $_(A_1, A_2N)()$ form a representation of $SL(2,ℤ)$ and the relation in [ref] [In fact, a slightly modified relation from [ref] is used in this paper, see equation [ref].] can be recovered by taking the limit $→exp(-2iπ/2N+3)$ under which $_(A_1, A_2N)()$ and $_(A_1, A_2N)()$ become the modular transformation matrices $S_(2N+3,2)$ and $T_(2N+3,2)$ of characters of $(2N+3,2)$ minimal models. $_(A_1, A_2N)()$ and $_(A_1, A_2N)()$ can be viewed as one parameter generalization of $S_(2N+3,2)$ and $T_(2N+3,2)$, and it will be shown in section [ref] that $_(A_1, A_2N)(
Argyres-Douglas Theories, Chiral Algebras and Wild Hitchin Characters · AD theories, wild Hitchin systems and VOAs · 0.83
Uses data or values from 1 paper
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Here we simply quote the result, [equation] where we replace the equivariant parameter $$ in [ref] by $=^1/2N+3$ for later convenience.
Argyres-Douglas Theories, Chiral Algebras and Wild Hitchin Characters · Coulomb branch index of $(A_1, A_2N)$ AD theories · 0.93
Compares with 2 papers
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In equation [ref] as in the original work of [ref] , the limit is taken to be $=e^2πi/2N+3$, whereas $=e^-2πi/2N+3$ in equation [ref] and [ref].
Argyres-Douglas Theories, Chiral Algebras and Wild Hitchin Characters · $(A_1,A_2)$ case · 0.88
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$N=4$, [equation] with [equation] and [equation] $ξ_i$'s are the diagonal elements of $_(11,2)$, [equation] The sign difference from [ref] in the above formula is originated from the sign difference in the $_(11,2)$.
Eigenvalue hypothesis for Racah matrices and HOMFLY polynomials for 3-strand knots in any symmetric and antisymmetric representations · S-matrix · 0.82
Cites as support 6 papers
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This was verified by matching the lens space Coulomb index of AD theories and the wild Hitchin characters [ref] , I_Coulomb ([Σ, G]; L(k,1)×S^1)= _ (Σ, ^LG_ℂ; k),
Equivariant Verlinde algebra from superconformal index and Argyres-Seiberg duality · AD theories, wild Hitchin systems and VOAs · 0.96
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This was verified by matching the lens space Coulomb index of AD theories and the wild Hitchin characters [ref] , I_Coulomb ([Σ, G]; L(k,1)×S^1)= _ (Σ, ^LG_ℂ; k),
Argyres-Douglas Theories, Chiral Algebras and Wild Hitchin Characters · AD theories, wild Hitchin systems and VOAs · 0.96
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Notice that the characters of $(2N+3,2)$ models are identified as the Schur indices with defect insertions of $(A_1, A_2N)$ AD theories [ref] .
Line defect Schur indices, Verlinde algebras and $U(1)_r$ fixed points · Conclusions and discussions · 0.96
Cites as background 13 papers
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Now recall the construction of $SU(N)$ refined CS theory [ref] .
Knot Homology from Refined Chern-Simons Theory · Relation with Refined Chern-Simons · 0.96
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An AD theory $$ can be constructed by compatifying $6d$ $(2,0)$ SCFT of type $G=ADE$ on a sphere $Σ$ with one irregular singularities and possible regular singularities [ref] .
Classification of Argyres-Douglas theories from M5 branes · AD theories, wild Hitchin systems and VOAs · 0.90
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An AD theory $$ can be constructed by compatifying $6d$ $(2,0)$ SCFT of type $G=ADE$ on a sphere $Σ$ with one irregular singularities and possible regular singularities [ref] .
Wild Quiver Gauge Theories · AD theories, wild Hitchin systems and VOAs · 0.90
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