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Singular instantons with SO(3) symmetry

2005/03/25 by Gregory D. Landweber, Landweber, Gregory D. · 1 citation
Mathematics · Physics and Astronomy · #53C07 #81T13 #Black Holes and Theoretical Physics #Differential Geometry (math.DG) #FOS: Mathematics #FOS: Physical sciences #Geometric and Algebraic Topology #Mathematical Physics (math-ph) #Noncommutative and Quantum Gravity Theories #math-ph #math.DG #math.MP #msc:53C07 #msc:81T13

paper · pdf · doi:10.48550/arxiv.math/0503611

26 pages

arxiv created 2005/03/25 · openalex publication_date 2005/03/25 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

This article provides an explicit construction for a family of singular instantons on S4 S2 with arbitrary real holonomy parameter α. This family includes the original α= 1/4, c2 = 3/2 solution discovered by P. Forgacs, Z. Horvath, and L. Palla, and our approach is modeled on that of their 1981 paper. Our primary tool is the ansatz due to Corrigan, Fairlie, Wilczek, and 't Hooft that constructs a self-dual Yang-Mills connection using a positive real-valued harmonic super-potential. Here we reformulate this harmonic function ansatz in terms of quaternionic notation, and we show that it arises naturally from the Levi-Civita connection of a conformally Euclidean metric. To simplify the construction, we introduce an SO(3)-action on S4, and we show by dimensional reduction that the symmetric self-duality equation on S4 is equivalent to the vortex equations over hyperbolic space H2. We thus obtain a similar harmonic function ansatz for hyperbolic vortices, which we also derive using conformal transformations of H2. Using this ansatz, we construct the vortex equivalents of the symmetric 't Hooft instantons, and we prove using the equivariant ADHM construction that they provide a complete description of all hyperbolic vortices. We also analyze when two vortices constructed by this ansatz are gauge equivalent, obtaining the surprising result that two such vortices are completely determined by the gauge transformation between them.

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