Are gravitating magnetic monopoles stable?
arXiv:1909.04205 · doi:10.1103/PhysRevD.100.063003
Abstract
The gravitating Julia-Zee dyon is a particle-like solution with both electric and magnetic charge. It is found in the Einstein-Yang-Mills-Higgs system of SU(2) with a scalar field in the adjoint representation coupled to gravity. Within the magnetic ansatz this system is reduced from describing dyons to describing the gravitating 't Hooft-Polyakov magnetic monopole. The stability of the well-known static gravitating magnetic monopole solutions with respect to perturbations within the magnetic ansatz--so-called magnetic perturbations--is well studied, but their stability with respect to perturbations outside the magnetic ansatz--so-called sphaleronic perturbations--is not. I undertake a purely numerical study by adding sphaleronic perturbations to gravitating magnetic monopole solutions and then dynamically evolving the system. For large perturbations I find that the system heads toward a dyon configuration, as expected. For sufficiently small perturbations, however, the system oscillates about the magnetic ansatz in a manner consistent with oscillations about a stable equilibrium.
12 pages, 5 figures
References in corpus (8)
- A hyperboloidal study of tail decay rates for scalar and Yang-Mills fields
- Saddle-point dynamics of a Yang-Mills field on the exterior Schwarzschild spacetime
- Formation and decay of Einstein-Yang-Mills black holes
- Critical phenomena in gravitational collapse with two competing massless matter fields
- Critical phenomena in the general spherically symmetric Einstein-Yang-Mills system
- Tails for the Einstein-Yang-Mills system
- Type II critical behavior of gravitating magnetic monopoles
- Stability and Critical Behavior of Gravitational Monopoles