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A Systematic Study on Matrix Models for Chern-Simons-matter Theories
High Energy Physics - Theory · Submitted 30 Apr 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This implies that many of Chern-Simons-matter theories have quite different properties from ABJM theory.
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The abstract, sentence by sentence
We investigate the planar solution of matrix models derived from various Chern-Simons-matter theories compatible with the planar limit. The saddle-point equations for most of such theories can be solved in a systematic way. A relation to Fuchsian systems play an important role in obtaining the planar resolvents. For those theories, the eigenvalue distribution is found to be confined in a bounded region even when the 't Hooft couplings become large. As a result, the vevs of Wilson loops are bounded in the large 't Hooft coupling limit. This implies that many of Chern-Simons-matter theories have quite different properties from ABJM theory. If the gauge group is of the form ${\rm U}(N_1)_{k_1}\times{\rm U}(N_2)_{k_2}$, then the resolvents can be obtained in a more explicit form than in the general cases.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate the planar solution of matrix models derived from various Chern-Simons-matter theories compatible with the planar limit. | contribution 1.00 | 0.93 | 0.06 | asserted 0.96 |
| s1 | The saddle-point equations for most of such theories can be solved in a systematic way. | method 0.57 | 0.66 | 0.07 | asserted 0.84 |
| s2 | A relation to Fuchsian systems play an important role in obtaining the planar resolvents. | method 0.97 | 0.52 | 0.06 | asserted 0.99 |
| s3 | For those theories, the eigenvalue distribution is found to be confined in a bounded region even when the 't Hooft couplings become large. | result 1.00 | 0.92 | 0.21 | asserted 1.00 |
| s4 | As a result, the vevs of Wilson loops are bounded in the large 't Hooft coupling limit. | result 0.95 | 0.86 | 0.22 | asserted 0.99 |
| s5 | This implies that many of Chern-Simons-matter theories have quite different properties from ABJM theory. | interpretation 1.00 | 0.68 | 0.39 | asserted 0.61 |
| s6 | If the gauge group is of the form ${\rm U}(N_1)_{k_1}\times{\rm U}(N_2)_{k_2}$, then the resolvents can be obtained in a more explicit form than in the general cases. | result 0.82 | 0.82 | 0.05 | asserted 0.95 |
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The paper
Original abstract
We investigate the planar solution of matrix models derived from various Chern-Simons-matter theories compatible with the planar limit. The saddle-point equations for most of such theories can be solved in a systematic way. A relation to Fuchsian systems play an important role in obtaining the planar resolvents. For those theories, the eigenvalue distribution is found to be confined in a bounded region even when the 't Hooft couplings become large. As a result, the vevs of Wilson loops are bounded in the large 't Hooft coupling limit. This implies that many of Chern-Simons-matter theories have quite different properties from ABJM theory. If the gauge group is of the form ${\rm U}(N_1)_{k_1}\times{\rm U}(N_2)_{k_2}$, then the resolvents can be obtained in a more explicit form than in the general cases.
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References
How the literature uses it
14 arXiv papers cite this in 21 sentences
Papers citing it · 9 sentences without a confident label
Builds on it 1 paper
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The analysis in this paper can be extended to a more general family of Chern-Simons-matter theories, based on the results obtained in [ref] .
Supersymmetry Breaking and Planar Free Energy in Chern-Simons-matter Theories · Introduction · 0.93
Cites it as background 9 papers
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The planar resolvents for such theories have been investigated in [ref] [ref] [ref] , however, explicit expressions for the resolvents have not been obtained so far except for ABJM theory and ABJ theory [ref] .
Notes on Planar Resolvents of Chern-Simons-matter Matrix Models · Introduction · 0.83
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The $S^3$ free energy of the GT theory has been computed in various ways: using resolvents in the 't Hooft limit [ref] ; using the saddle point approximation of a matrix model [ref] and in the Fermi-gas approach in the large-$N$ limit with fixed Chern-Simons levels [ref] .
Subleading corrections to the $S^3$ free energy of necklace quiver theories dual to massive IIA · Introduction · 0.96
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However, if we consider more general M2-brane theory beyond[ For previous studies, see e.g. [ref] in the M-theory limit, [ref] in the 't Hooft limit and [ref] in the Fermi gas approach. ] the ABJ(M) theory, the correspondence to the topological string is rather obscure, and it might be the case that there is no such relation in general.
Exact results on ABJ theory and the refined topological string · Discussions · 0.94
What it cites · 53 sentences without a confident label
Builds on 3 papers
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To clarify the situation, it is desired to extend the analysis in [ref] to more general theories.
On Large N Solution of N=3 Chern-Simons-adjoint Theories · Introduction · 0.93
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The relation to a Fermi gas can be extended [ref] to various Chern-Simons-matter theories of quiver types originally studied in [ref] .
Multi-Matrix Models and Tri-Sasaki Einstein Spaces · Introduction · 0.92
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The relation to a Fermi gas can be extended [ref] to various Chern-Simons-matter theories of quiver types originally studied in [ref] .
ABJM theory as a Fermi gas · Introduction · 0.92
Uses the method or tool of 4 papers
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For most of these theories, the Fermi gas approach [ref] results in interacting theories.
ABJM theory as a Fermi gas · Introduction · 0.90
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It was found in [ref] that the following ansatz [equation] for the resolvents is quite useful to deal with the logarithmic functions.
On Large N Solution of N=3 Chern-Simons-adjoint Theories · Integral ansatz · 0.96
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Using the supersymmetric localization [ref] , $Z(Γ)$ can be written in terms of a finite-dimensional Riemann integral.
Exact Results for Wilson Loops in Superconformal Chern-Simons Theories with Matter · Saddle-point equations for theories in $C$ · 0.89
Compares with 6 papers
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The same formula was also derived in [ref] in a different way.
ABJM theory as a Fermi gas · Introduction · 0.90
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These theories are rather similar to the Chern-Simons-adjoint theories investigated in [ref] .
On Large N Solution of N=3 Chern-Simons-adjoint Theories · Discussion · 0.96
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Similar results were found in [ref] .
Interacting fermions and N=2 Chern-Simons-matter theories · 't Hooft couplings · 0.92
Cites as background 14 papers
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In this limit, one finds a relation to M-theory on AdS$_4×S^7/ℤ_k$ [ref] in a quite similar way to the well-studied AdS$_5$/CFT$_4$ correspondence [ref] .
N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals · Introduction · 0.88
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In [ref] , $N=3$ Chern-Simons-adjoint theories were discussed.
On Large N Solution of N=3 Chern-Simons-adjoint Theories · Chern-Simons-adjoint theory revisited · 0.95
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The worldvolume theory on M2-branes in the flat space-time was constructed in [ref] [ref] [ref] [ref] [ref] whose applicability is, however, limited to the system with two M2-branes.
Selfdual strings and loop space Nahm equations · Introduction · 0.90
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