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Simple Singularities and N=2 Supersymmetric Yang-Mills Theory
High Energy Physics - Theory · Submitted 7 Nov 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Specifically, we propose a particular sequence of hyperelliptic genus $n-1$ Riemann surfaces to underly the quantum moduli space of $SU(n)$ N=2 supersymmetric gauge theory.
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The abstract, sentence by sentence
We present a first step towards generalizing the work of Seiberg and Witten on N=2 supersymmetric Yang-Mills theory to arbitrary gauge groups. Specifically, we propose a particular sequence of hyperelliptic genus $n-1$ Riemann surfaces to underly the quantum moduli space of $SU(n)$ N=2 supersymmetric gauge theory. These curves have an obvious generalization to arbitrary simply laced gauge groups, which involves the A-D-E type simple singularities. To support our proposal, we argue that the monodromy in the semiclassical regime is correctly reproduced. We also give some remarks on a possible relation to string theory.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a first step towards generalizing the work of Seiberg and Witten on N=2 supersymmetric Yang-Mills theory to arbitrary gauge groups. | contribution 0.73 | 0.83 | 0.11 | asserted 0.96 |
| s1 | Specifically, we propose a particular sequence of hyperelliptic genus $n-1$ Riemann surfaces to underly the quantum moduli space of $SU(n)$ N=2 supersymmetric gauge theory. | contribution 0.97 | 0.90 | 0.38 | asserted 0.45 |
| s2 | These curves have an obvious generalization to arbitrary simply laced gauge groups, which involves the A-D-E type simple singularities. | contribution 0.87 | 0.66 | 0.17 | asserted 0.99 |
| s3 | To support our proposal, we argue that the monodromy in the semiclassical regime is correctly reproduced. | result 0.84 | 0.86 | 0.13 | asserted 0.81 |
| s4 | We also give some remarks on a possible relation to string theory. | interpretation 0.65 | 0.68 | 0.03 | hedged possibility 0.84 |
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The paper
Original abstract
We present a first step towards generalizing the work of Seiberg and Witten on N=2 supersymmetric Yang-Mills theory to arbitrary gauge groups. Specifically, we propose a particular sequence of hyperelliptic genus $n-1$ Riemann surfaces to underly the quantum moduli space of $SU(n)$ N=2 supersymmetric gauge theory. These curves have an obvious generalization to arbitrary simply laced gauge groups, which involves the A-D-E type simple singularities. To support our proposal, we argue that the monodromy in the semiclassical regime is correctly reproduced. We also give some remarks on a possible relation to string theory.
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References
How later papers used it
46 later papers cite it
1 paper by the same authors is listed below: 1 built on it.
Builds on it 1 of 2 papers with this label · 1 by the same authors
By the same authors
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Based the first term in its curve on this paper's pure SU(N) generalization.
The Omega deformed B-model for rigid N=2 theories (2011) (same authors) · 0.90 · paraphrased: the licence does not allow quoting
How the literature uses it
45 arXiv papers cite this in 69 sentences
Papers citing it · 41 sentences without a confident label
Contests it 1 paper
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For this, one needs to match the $F_4$ expansions with the leading coefficients of the (differentiated) prepotential [ref] = τ_0/6∑_i=1^3Z_i^2+_1-loop+_inst., where[We correct a typo in [ref] .] τ_0 =9-log4/2πi.
Elliptic Loci of SU(3) Vacua · Picard-Fuchs system for large $v$ · contest 0.90
Builds on it 2 papers
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The general-$N$ statements (sw_curve_admits_effective_theory, sw_effective_theory_unique_up_to_duality, extended to $SU(N)$ in [ref] ) are proved in the same repository from one consolidated period input, periodRigidityAxiom (the Gauss–Manin / Picard–Fuchs period-variation theorem); constructing that higher-genus period geometry is future work (6, B.1).
Axioms for physical reasoning: codifying the Seiberg--Witten solution in Lean · What is proved · 0.83
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The first term in this curve is based on the pure $SU(N)$ generalization [ref] [ref] of [ref] , while the mass dependent terms are fixed by requiring the correct residua of the Seiberg-Witten differential.
The Omega deformed B-model for rigid N=2 theories · The $SU(N)$ $N_f=2N$ curves · 0.90
Uses its method or tool 2 papers
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The metric on the moduli space can be computed from the curve $C$ [ref] :
Non Supersymmetric Metastable Vacua in N=2 SYM Softly Broken to N=1 · $SU(3)$ $N=2$ SYM with flavor · 0.89
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In appendix [ref] we derive $(a^(N_F,k)_D,a^(N_F,k))$ and $F^(N_F,k)$ using the latter method, following [ref] , and in particular the solutions in particular [ref] .
Phase Transitions at Unusual Values of $\theta$ · Singularity Structure · 0.97
Compares with it 1 paper
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We note that is also the Weierstrass form for the Seiberg-Witten curve for pure $SU(2)$ gauge theory as quoted in [ref] , while if we transform the $N_f=0$ case [ref] in ([ref]) into Weierstrass form we obtain [equation] The two curves specified by ([ref]) with ([ref]) or ([ref]) respectively are known to be isogeneous.
Holomorphicity and Modularity in Seiberg-Witten Theories with Matter · Review of the formalism · 0.90
Cites it as background 17 papers
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As is well known from the work of Seiberg and Witten [ref] and its generalizations [ref] , the low-energy description of the $=2$ theory involves a Coulomb branch of vacua, parametrized by $N-1$ holomorphic moduli $u_I = (ϕ^I)$ with $I=2, …, N$.
Cascading from $\mathscr{N}=2$ Supersymmetric Yang-Mills Theory to Confinement and Chiral Symmetry Breaking in Adjoint QCD · The small-SUSY-breaking regime: $M ≪Λ$ · 0.91
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The low energy effective theory (and the quantum Coulomb moduli space) of $=2$ supersymmetric gauge theory is described by the Seiberg-Witten curve and the meromorphic one-form called Seiberg-Witten one-form [ref] .
The Quiver Matrix Model and 2d-4d Conformal Connection · $=2$ gauge theory and Seiberg-Witten curve · 0.97
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We first recall the Seiberg-Witten geometry in Section [ref] following [ref] .
Elliptic Loci of SU(3) Vacua · The Coulomb branch of the $SU(3)$ theory · 0.89
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