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Oscillons in the broken vacuum and global vortex annihilation

D. Canillas Martínez, A. González-Parra, D. Miguélez-Caballero, A. Wereszczynski

Abstract

In contrast to the complex $φ^4$ model, vortex-antivortex collisions in the complex $φ^6$ theory reveal a resonant structure due to the existence of a remarkably stable, long-lived, large amplitude oscillon in the broken vacuum. Surprisingly, it persists despite the absence of a mass gap associated with the flat direction in the broken vacuum. We demonstrate that its existence is related to a far-distance modification of the potential, namely, the appearance of an unbroken (false or true) vacuum.

Oscillons in the broken vacuum and global vortex annihilation

Abstract

In contrast to the complex model, vortex-antivortex collisions in the complex theory reveal a resonant structure due to the existence of a remarkably stable, long-lived, large amplitude oscillon in the broken vacuum. Surprisingly, it persists despite the absence of a mass gap associated with the flat direction in the broken vacuum. We demonstrate that its existence is related to a far-distance modification of the potential, namely, the appearance of an unbroken (false or true) vacuum.

Paper Structure

This paper contains 10 sections, 18 equations, 10 figures.

Figures (10)

  • Figure 1: Profiles of the unit charge vortices in the $\phi^4$ (blue curve) and $\phi^6$ models (orange curve).
  • Figure 2: The VAV collision. Energy density at the origin as a function of time for various values of the initial velocity $v_{\rm in}$. Upper panel: $\phi^6$ model. Lower panel: $\phi^4$ model.
  • Figure 3: Formation of a radially symmetric oscillon in the VAV collision in the $\phi^6$ model with $v_{\rm in}=0$ and $2d=20$.
  • Figure 4: The real and imaginary component of $\phi$ at the origin in the VAV collision with $v_{\rm in}=0$ and $d=20$. Upper: oscillon formation in the $\phi^6$ theory. Lower: Absence of oscillon in the complex $\phi^4$ theory.
  • Figure 5: Evolution of the normalized energy enclosed in the disc with radius $R=d/2$ for the VAV collision with $v_{\rm in}=0$ in the $\phi^6$ (blue) and $\phi^4$ (green) models and for the perturbed Gaussian initial data (orange).
  • ...and 5 more figures