General bubble expansion at strong coupling

Wang, Jun-Chen, Yuwen, Zi-Yan, Hao, Yu-Shi, Wang, Shao-Jiang
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Abstract

The strongly-coupled system like the quark-hadron transition (if it is of first order) is becoming an active play-yard for the physics of cosmological first-order phase transitions. However, the traditional field theoretic approach to strongly-coupled first-order phase transitions is of great challenge, driving recent efforts from holographic dual theories with explicit numerical simulations. These holographic numerical simulations have revealed an intriguing linear correlation between the phase pressure difference (pressure difference away from the wall) to the non-relativistic terminal velocity of an expanding planar wall, which has been reproduced analytically alongside both cylindrical and spherical walls from perfect-fluid hydrodynamics in our previous study but only for a bag equation of state. We have also found in our previous study a universal quadratic correlation between the wall pressure difference (pressure difference near the bubble wall) to the non-relativistic terminal wall velocity regardless of wall geometries. In this paper, we will generalize these analytic relations between the phase/wall pressure difference and terminal wall velocity into a more realistic equation of state beyond the simple bag model, providing the most general predictions so far for future tests from holographic numerical simulations of strongly-coupled first-order phase transitions
一般气泡在强耦合时膨胀
然而,传统的场理论方法对强耦合一阶相变是巨大的挑战,推动了最近全息对偶理论与显式数值模拟的努力。这些全息数值模拟揭示了相压差(远离壁面的压力差)与膨胀平面壁面的非相对论性终端速度之间有趣的线性关系,这在我们之前的研究中已经从完美流体力学中解析地再现了圆柱形和球形壁面,但仅适用于袋状态方程。我们在之前的研究中还发现,无论壁面几何形状如何,壁面压力差(气泡壁面附近的压力差)与非相对论性末端壁面速度之间存在普遍的二次相关关系。在本文中,我们将这些相/壁压差和终端壁速度之间的解析关系推广到一个更现实的状态方程中,超越简单的袋模型,为强耦合一阶相变的全息数值模拟的未来测试提供迄今为止最一般的预测
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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