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All Exact Solutions of Non-Abelian Vortices from Yang-Mills Instantons
High Energy Physics - Theory · Submitted 21 Jul 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We successfully exhaust the complete set of exact solutions of non-Abelian vortices in a quiver gauge theory, that is, the S[U(N) x U(N)] gauge theory with a bi-fudamental scalar field on a hyperbolic plane with a certain curvature, from SO(3)-invariant SU(2N) Yang-Mills instanton solutions.
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The abstract, sentence by sentence
We successfully exhaust the complete set of exact solutions of non-Abelian vortices in a quiver gauge theory, that is, the S[U(N) x U(N)] gauge theory with a bi-fudamental scalar field on a hyperbolic plane with a certain curvature, from SO(3)-invariant SU(2N) Yang-Mills instanton solutions. This work provides, for the first time, exact non-Abelian vortex solutions. We establish the ADHM construction for non-Abelian vortices and identify all the moduli parameters and the complete moduli space.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We successfully exhaust the complete set of exact solutions of non-Abelian vortices in a quiver gauge theory, that is, the S[U(N) x U(N)] gauge theory with a bi-fudamental scalar field on a hyperbolic plane with a certain curvature, from SO(3)-invariant SU(2N) Yang-Mills instanton solutions. | contribution 0.52 | 0.95 | 0.78 | asserted 1.00 |
| s1 | This work provides, for the first time, exact non-Abelian vortex solutions. | contribution 0.63 | 0.93 | 0.30 | asserted 1.00 |
| s2 | We establish the ADHM construction for non-Abelian vortices and identify all the moduli parameters and the complete moduli space. | contribution 0.70 | 0.95 | 0.21 | asserted 1.00 |
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The paper
Original abstract
We successfully exhaust the complete set of exact solutions of non-Abelian vortices in a quiver gauge theory, that is, the S[U(N) x U(N)] gauge theory with a bi-fudamental scalar field on a hyperbolic plane with a certain curvature, from SO(3)-invariant SU(2N) Yang-Mills instanton solutions. This work provides, for the first time, exact non-Abelian vortex solutions. We establish the ADHM construction for non-Abelian vortices and identify all the moduli parameters and the complete moduli space.
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How the literature uses it
5 arXiv papers cite this in 5 sentences
Papers citing it · 3 sentences without a confident label
Cites it as background 2 papers
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Important generalizations of BPS vortices have been studied in curved space, such as hyperbolic space [ref] and general Riemann surfaces [ref] .
Higgs and Coulomb Branch Descriptions of the Volume of the Vortex Moduli Space · Introduction · 0.92
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Recent progress for integrable vortex models are found in [ref] .
BPS Boojums in N=2 supersymmetric gauge theories I · Introduction and summary · 0.98
What it cites · 5 sentences without a confident label
Builds on 1 paper
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Here, we extend this relation to the non-Abelian case [ref] .
Maximally Non-Abelian Vortices from Self-dual Yang--Mills Fields · $SU(2N)$ instanton to $S[U(N) ×U(N)]$ vortices · 0.99
Cites as background 7 papers
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Non-Abelian vortices also play prominent roles as instantons in non-perturbative dynamics of gauge theories in lower dimensions, similar to the role of Yang-Mills instantons [ref] in four dimensions; the non-perturbative partition function has been extensively studied by the vortex counting in $N=(2,2)$ supersymmetric gauge theories in two dimensions [ref] , similar to the instanton counting in four dimensions [ref] .
Vortex Counting and Lagrangian 3-manifolds · Introduction · 0.81
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The asymptotic metric for well-separated vortices was obtained [ref] to study the low-energy scattering [ref] .
Dynamics of Non-Abelian Vortices · Introduction · 0.88
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The asymptotic metric for well-separated vortices was obtained [ref] to study the low-energy scattering [ref] .
The Moduli Space Metric for Well-Separated Non-Abelian Vortices · Introduction · 0.88
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