<p>We show that, in the thin-wall regime, <i>Q</i>-ball-anti-<i>Q</i>-ball collisions reveal chaotic behaviour. This is explained by the resonant energy transfer mechanism triggered by the internal modes hosted by the <i>Q</i>-balls and by the existence of <i>ephemeral</i> states, that is unstable, sometimes even short-lived, field configurations that appear as intermediate states. The most important examples of such states are the <i>bubble</i> of the false broken vacuum, which as intermediate states govern the <i>QQ</i><sup>*</sup> annihilation, and the <i>charged oscillons</i>.</p><p>The usually short-lived bubble can be dynamically temporarily stabilized, which explains their importance in the dynamics of <i>Q</i>-balls. This happens due to the excitation of massless Goldstone modes, which, exerting pressure on the bubble boundaries or being trapped as bound modes, prevent the bubble from collapsing.</p>

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Oscillons and bubbles in Q-ball dynamics

  • D. Canillas Martínez,
  • P. Dorey,
  • T. Romańczukiewicz,
  • Paul M. Saffin,
  • K. Sławińska,
  • A. Wereszczyński

摘要

We show that, in the thin-wall regime, Q-ball-anti-Q-ball collisions reveal chaotic behaviour. This is explained by the resonant energy transfer mechanism triggered by the internal modes hosted by the Q-balls and by the existence of ephemeral states, that is unstable, sometimes even short-lived, field configurations that appear as intermediate states. The most important examples of such states are the bubble of the false broken vacuum, which as intermediate states govern the QQ* annihilation, and the charged oscillons.

The usually short-lived bubble can be dynamically temporarily stabilized, which explains their importance in the dynamics of Q-balls. This happens due to the excitation of massless Goldstone modes, which, exerting pressure on the bubble boundaries or being trapped as bound modes, prevent the bubble from collapsing.