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Spherically symmetric Dirac-Yang-Mills pairs on Riemannian 3-manifolds

Adam Lindström, Marko Sobak

TL;DR

This work constructs spherically symmetric Dirac-Yang-Mills pairs with structure group $SU(2)$ on 3-manifolds of the form $M = N\times\mathbb{S}^2$ by developing an invariant bundle framework and an invariant spinor/gauge ansatz. The authors reduce the DYM equations to a tractable system of ordinary differential equations using a polar decomposition and a detailed invariant-spinor analysis, yielding explicit global solutions and a rich family of coupled, periodically-reducing configurations. They identify regimes with constant spinor-norm $\rho$ (and two distinct regimes $\delta_0=0$ and $\delta_0>0$), obtaining explicit solutions, singular behavior, and conditions under which solutions descend to closed manifolds like $\mathbb{S}^1\times\mathbb{S}^2$. The results provide the first known examples of coupled DYM pairs on closed Riemannian spin manifolds and demonstrate the feasibility of generating entire families of periodic DYM configurations by a carefully chosen spherically symmetric ansatz. The constructions have potential implications for geometric models of gauge-fermion interactions and offer a concrete setting to explore variational and topological aspects of DYM systems on curved spaces.

Abstract

In this paper we construct examples of spherically symmetric Dirac-Yang-Mills pairs on Riemannian 3-manifolds with the structure group SU(2). This approach yields coupled solutions (i.e. the connection is not a Yang-Mills connection) and among them are solutions on S^1(r_1) x S^2(r_2) for certain radii r_1 and r_2. These are, to the authors' best knowledge, the first examples of coupled Dirac-Yang-Mills pairs on a closed Riemannian spin manifold.

Spherically symmetric Dirac-Yang-Mills pairs on Riemannian 3-manifolds

TL;DR

This work constructs spherically symmetric Dirac-Yang-Mills pairs with structure group on 3-manifolds of the form by developing an invariant bundle framework and an invariant spinor/gauge ansatz. The authors reduce the DYM equations to a tractable system of ordinary differential equations using a polar decomposition and a detailed invariant-spinor analysis, yielding explicit global solutions and a rich family of coupled, periodically-reducing configurations. They identify regimes with constant spinor-norm (and two distinct regimes and ), obtaining explicit solutions, singular behavior, and conditions under which solutions descend to closed manifolds like . The results provide the first known examples of coupled DYM pairs on closed Riemannian spin manifolds and demonstrate the feasibility of generating entire families of periodic DYM configurations by a carefully chosen spherically symmetric ansatz. The constructions have potential implications for geometric models of gauge-fermion interactions and offer a concrete setting to explore variational and topological aspects of DYM systems on curved spaces.

Abstract

In this paper we construct examples of spherically symmetric Dirac-Yang-Mills pairs on Riemannian 3-manifolds with the structure group SU(2). This approach yields coupled solutions (i.e. the connection is not a Yang-Mills connection) and among them are solutions on S^1(r_1) x S^2(r_2) for certain radii r_1 and r_2. These are, to the authors' best knowledge, the first examples of coupled Dirac-Yang-Mills pairs on a closed Riemannian spin manifold.
Paper Structure (26 sections, 7 theorems, 171 equations, 3 figures, 2 tables)

This paper contains 26 sections, 7 theorems, 171 equations, 3 figures, 2 tables.

Key Result

Theorem 1.1

Let $N = \mathbb{R}$ or $N = \mathbb{S}^1$. Then in both cases, there exist families of spherically symmetric Riemannian metrics $g$ on $N\times \mathbb{S}^2$ admitting globally defined coupled spherically symmetric Dirac-Yang-Mills pairs with structure group $\mathbf{SU}(2)$.

Figures (3)

  • Figure 1: Solutions $W(s)$ of \ref{['eq-W-delta=0-rho<1']}.
  • Figure 2: Phase portrait of \ref{['eq-P-W-system-delta0>0-rho0<1']}.
  • Figure 4: Phase portrait of \ref{['eq-autonomous-kappa-pos']} for $\lambda=1$, $\beta=\sqrt{7/8}$, $\alpha=2$. The green (resp. red) curve represents the stable (resp. unstable) manifold at the fixed point $(\alpha,0)$. The blue curves are the global solutions lying in the region $D_+ \cup D_-$. The brown curves are some prototypical orbits that do not lie entirely in $D_+ \cup D_-$, they all have $x \to 0$ at some finite $s$ (either forwards or backwards or both).

Theorems & Definitions (16)

  • Theorem 1.1
  • Remark 2.1
  • Remark 2.2
  • Remark 3.1
  • Lemma 3.2
  • proof
  • Lemma 3.3: Polar form
  • Remark 3.4
  • Proposition 4.1: The case $\delta_0 = 0$
  • Remark 4.2
  • ...and 6 more