Here we present supplementary online video material concerning the following publication:
Thomas Gasenzer, Boris Nowak, and Denes Sexty
1Institut für Theoretische Physik, Ruprecht-Karls-Universität Heidelberg, Philosophenweg 16, 69120 Heidelberg, Germany
2ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, 64291 Darmstadt, Germany
New aspects of parametrically resonant heating of a relativistic scalar O(2)-symmetric self-interacting field are presented. This process is a candidate for reheating at the end of the early-universe epoch of inflation. Although a model with a fully O(2)-symmetric ground state is used, transient, metastable spontaneous symmetry breaking can be observed. This manifests itself in the form of persistent regimes of opposite and, inside these, uniform charge overdensities separated by thin lines and walls similar to topological defects, in two and three spatial dimensions, respectively. The configuration is found to correspond to an attractive non-equilibrium fixed point of the underlying dynamic equations which prevents thermalisation over an extended period of time.
arXiv:1108.0541 [hep-ph]
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Videos by Dénes Sexty
The videos show a 2D simulation of the 2-component relativistic scalar field according to the O(2)-symmetric Klein-Gordon model with λ(φcφc)2 non-linear interactions.
To induce the shown parametrically resonant reheating, we start our simulations from a configuration where only the zero mode of the inflaton field φ is populated. Fluctuating non-zero momentum modes act as seeds for the ensuing instabilities. Choosing the mass-squared m2 = 0 and λ > 0, which corresponds to an equilibrium configuration in the symmetric phase, subsequent oscillation of the inflaton field induces parametrically resonant exponential growth of certain modes. Scattering between these modes causes the entire spectrum to fill up.
Looking at the real-space structure of the emerging critical configuration we find patterns similar to topo- logical defects giving rise to quasi-stationary charge separation. We find a correspondence between the appearance of the strong scaling exponent and of the defect-separated charge patterns. In Figure 2 in the above paper we depict, for d = 2, a typical real-space configuration in the turbulent stage, plotting the modulus of the O(2) scalar field, |Φ(x,t)| = [Φ12(x,t) + Φ22(x,t)]1/2. Localised regions appear, specifically “defect” lines where the absolute value of the field is much smaller than its average. Fig. 3 in the paper shows the corresponding charge density ρ(x,t) = j0(x,t), Eq. (4). Clearly, both uniform charge and anti-charge overdensities appear within distinctly separated regions, showing only small fluctuations as compared to their bulk values. This separation of charges is confirmed by the histogram of local charge densities shown in Fig. 4 in the paper.
Video of the whole evolution from t=0 to t=10000, illustrating the slowly evolving, reconnecting defect lines. Plotted is rho, gradient energy density, charge density.
The time evolution of the defect lines and the particle number spectrum.
The bubble wall: In a 3d simulation on a 64^3 lattice, at t=1500, points with rho^2<0.05 are higlighted:
Time evolution of the 3d system from t=0 to t=4700. Points with rho^2<0.05 are highlighted.
