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A Large N Duality via a Geometric Transition
High Energy Physics - Theory · Submitted 9 Mar 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This duality yields highly non-trivial exact results for the gauge theory.
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The abstract, sentence by sentence
We propose a large N dual of 4d, N=1 supersymmetric, SU(N) Yang-Mills with adjoint field \Phi and arbitrary superpotential W(\Phi). The field theory is geometrically engineered via D-branes partially wrapped over certain cycles of a non-trivial Calabi-Yau geometry. The large N, or low-energy, dual arises from a geometric transition of the Calabi-Yau, where the branes have disappeared and have been replaced by suitable fluxes. This duality yields highly non-trivial exact results for the gauge theory. The predictions indeed agree with expected results in cases where it is possible to use standard techniques for analyzing the strongly coupled, supersymmetric gauge theories. Moreover, the proposed large N dual provides a simpler and more unified approach for obtaining exact results for this class of supersymmetric gauge theories.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We propose a large N dual of 4d, N=1 supersymmetric, SU(N) Yang-Mills with adjoint field \Phi and arbitrary superpotential W(\Phi). | contribution 1.00 | 0.89 | 0.48 | asserted 0.72 |
| s1 | The field theory is geometrically engineered via D-branes partially wrapped over certain cycles of a non-trivial Calabi-Yau geometry. | method 0.93 | 0.51 | 0.05 | asserted 1.00 |
| s2 | The large N, or low-energy, dual arises from a geometric transition of the Calabi-Yau, where the branes have disappeared and have been replaced by suitable fluxes. | method 0.78 | 0.53 | 0.31 | asserted 1.00 |
| s3 | This duality yields highly non-trivial exact results for the gauge theory. | result 0.74 | 0.76 | 0.32 | asserted 1.00 |
| s4 | The predictions indeed agree with expected results in cases where it is possible to use standard techniques for analyzing the strongly coupled, supersymmetric gauge theories. | result 0.95 | 0.62 | 0.11 | asserted 0.90 |
| s5 | Moreover, the proposed large N dual provides a simpler and more unified approach for obtaining exact results for this class of supersymmetric gauge theories. | interpretation 0.74 | 0.70 | 0.29 | asserted 0.99 |
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The paper
Original abstract
We propose a large N dual of 4d, N=1 supersymmetric, SU(N) Yang-Mills with adjoint field \Phi and arbitrary superpotential W(\Phi). The field theory is geometrically engineered via D-branes partially wrapped over certain cycles of a non-trivial Calabi-Yau geometry. The large N, or low-energy, dual arises from a geometric transition of the Calabi-Yau, where the branes have disappeared and have been replaced by suitable fluxes. This duality yields highly non-trivial exact results for the gauge theory. The predictions indeed agree with expected results in cases where it is possible to use standard techniques for analyzing the strongly coupled, supersymmetric gauge theories. Moreover, the proposed large N dual provides a simpler and more unified approach for obtaining exact results for this class of supersymmetric gauge theories.
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References
How later papers used it
49 later papers cite it
2 later papers by other authors are listed below: 2 used its method or tool.
Uses its method or tool 2 of 10 papers with this label
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Computed each term in the series explicitly and gave it most easily in terms of a generating function from this paper.
Direct Integration and Non-Perturbative Effects in Matrix Models (2010) · 0.89 · paraphrased: the licence does not allow quoting
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Used a convenient reparametrization with two complex parameters first introduced in this paper.
Large N instantons from topological strings (2023) · 0.85 · paraphrased: the licence does not allow quoting
How the literature uses it
48 arXiv papers cite this in 104 sentences
Papers citing it · 55 sentences without a confident label
Builds on it 1 paper
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It is actually the celebrated CIV-DV prepotential [ref] , just modified (generalized) in three different directions: from polynomial to logarithmic potential $V$, to $β≠1$ and to arbitrary genus.
The matrix model version of AGT conjecture and CIV-DV prepotential · Conclusion · 0.86
Uses its method or tool 10 papers
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The analysis of the more interesting $SU(N)$ case along these lines requires the use of the Dijkgraaf-Vafa superpotential [ref] , which allows us to capture all the holomorphic data of the theory by means of a planar calculation in a matrix model, and of the generalized Konishi anomaly [ref] .
Confining vacua in SQCD, the Konishi anomaly and the Dijkgraaf-Vafa superpotential · Introduction · 1.00
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$∙$Another side of equality is the same integral, but treated differently: as Givental decomposition [ref] into a system of Gaussian models with the filling numbers $(N_1,…,N_r)$.
The matrix model version of AGT conjecture and CIV-DV prepotential · Conclusion · 0.80
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The analysis of the more interesting $SU(N)$ case along these lines requires the use of the Dijkgraaf-Vafa superpotential [ref] , which allows us to capture all the holomorphic data of the theory by means of a planar calculation in a matrix model, and of the generalized Konishi anomaly [ref] .
Confinement and duality in supersymmetric gauge theories · Introductory remarks · 0.99
Compares with it 4 papers
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As we discussed around diff we can define a bare scale parameter as $Λ̂= ρ_c /√(α' M)$, and then, to compare directly with with [ref] , let us also define $S=e^-t_∞- i ψ_∞$ and a “complex coupling” $2πα' α̃= -(j+i b)$.
The unwarped, resolved, deformed conifold: fivebranes and the baryonic branch of the Klebanov-Strassler theory · The superpotential · 0.87
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8pt0pt + ∑_a ≠b 1Δ_aΔ_b ( S_aS_b(4S_a^2 + 11S_a S_b + 4S_b^2) 4(μ_a - μ_b)^4 - ∑_c ≠a_d ≠b S_a S_b(S_a + S_c)(S_b + S_d)2 (μ_a - μ_b)^2 (μ_a - μ_c) (μ_b - μ_d) - ∑_c ≠b S_aS_b(S_a+2S_b)(S_b+S_c) (μ_a - μ_b)^3 (μ_b - μ_c) ) These formulas reproduce and generalise various explicit results, available in the literature [ref] , in particular the cubic contribution coincides with the one obtained in [ref] by different methods.
The matrix model version of AGT conjecture and CIV-DV prepotential · The case of $β= 1$ and genus zero: ordinary CIV-DV prepotential · 0.90
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This is to be contrasted with the case of pure $𝒩 = 1$ $SU(N)$ gauge theory engineered from D5-branes wrapping a rigid $ℙ^1$ in a local Calabi-Yau 3-fold as in [ref] , where the corresponding volume modulus is non-dynamical.
Instantons and SUSY breaking in F-theory · Introduction · 0.99
Cites it as support 1 paper
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This chain of results, together with large $r$ duality [ref] , strongly supports a 6d version of the AGT correspondence by identifying generic chiral blocks of the elliptic Virasoro algebra with $ℝ^4×𝕋^2$ Nekrasov instanton partition functions.
An elliptic Virasoro symmetry in 6d · Introduction · 0.96
Cites it as background 24 papers
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It has been conjectured in the context of the topological string theory and the gauge/gravity correspondence [ref] that the effective superpotential is related to the matrix model free energy [ref] , which we refer to as Dijkgraaf-Vafa relation.
Deformation of Dijkgraaf-Vafa Relation via Spontaneously Broken N=2 Supersymmetry II · Introduction · 0.83
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In this appendix, we first review different approaches to computing the prepotential $_0$ for the Dijkgraaf-Vafa (CIV-DV) geometries [ref] given in eqs.
Nonsupersymmetric Flux Vacua and Perturbed N=2 Systems · Prepotential for Dijkgraaf-Vafa (CIV-DV) Geometries · 0.99
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[equation] Such models have been studied for quite a long time: in the case, when $V(z)$ is a polynomial, their free energy $F = logZ$ gives rise to the CIV-DV prepotential [ref] .
The matrix model version of AGT conjecture and CIV-DV prepotential · $ħ$-expansion for the generic case · 0.88
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