ArXiv TLDR

Exact SU(2) Yang-Mills Waves from a Simple Ansatz

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2605.04964

Yu-Xuan Zhang, Jing-Ling Chen

quant-phhep-thmath-ph

TLDR

This paper proposes a simple ansatz to construct three families of exact wave solutions for sourceless SU(2) Yang-Mills equations.

Key contributions

  • Proposes a simple ansatz using a rotated Pauli basis to solve SU(2) Yang-Mills equations.
  • Identifies three families of exact wave solutions, including linear and genuinely nonlinear types.
  • Family II describes nonlinear, self-interacting waves with a constant field offset and non-zero time-averaged color-electric field.
  • Nonlinear waves propagate at light speed, do not superpose, and have energy density nodes controlled by a topological parameter.

Why it matters

This work provides new, closed-form solutions for SU(2) Yang-Mills waves, offering crucial insights into how non-Abelian self-interactions fundamentally alter wave propagation. It reveals observable signatures like energy density nodes and a non-zero time-averaged color-electric field.

Original Abstract

We propose a simple ansatz to construct exact wave solutions of the sourceless SU(2) Yang-Mills equations in (3+1) dimensions. The ansatz employs a $y$-dependent rotated Pauli basis and assumes a phase $θ=kz-ωt$ dependence for the gauge potentials. Owing to this ansatz, the nonlinear field equations reduce to nine algebraic constraints, whose complete solution yields three families of exact waves. Family I describes linear (Abelian) electromagnetic waves embedded in the non-Abelian theory; all commutator terms vanish and the dispersion relation is $ω=kc$. Family II represents genuinely nonlinear self-interacting waves that also propagate at the speed of light but exhibit a constant field offset, nonvanishing commutators, and do not obey superposition. The constant offset is gauge-invariant and gives rise to a non-zero time-averaged color-electric field. The energy density has nodes whose position ($θ=0$ or $θ=π$) is controlled by a discrete topological parameter $ξη=\pm1$, providing an observable signature. Family III is a pure gauge solution with vanishing field strengths, valid for arbitrary $k$ and $ω$ without any dispersion relation. All solutions are closed-form and provide new insights into how non-Abelian self-interactions fundamentally alter wave propagation.

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