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Quantum chaos, thermalization, and entanglement generation in real-time simulations of the Banks-Fischler-Shenker-Susskind matrix model

机译:Banks-Fischler-Shenker-Susskind矩阵模型的实时仿真中的量子混沌,热化和纠缠生成

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We study numerically the onset of chaos and thermalization in the Banks-Fischler-Shenker-Susskind (BFSS) matrix model with and without fermions, considering Lyapunov exponents, entanglement generation, and quasinormal ringing. We approximate the real-time dynamics in terms of the most general Gaussian density matrices with parameters which obey self-consistent equations of motion, thus extending the applicability of real-time simulations beyond the classical limit. Initial values of these Gaussian density matrices are optimized to be as close as possible to the thermal equilibrium state of the system. Thus attempting to bridge between the low-energy regime with a calculable holographic description and the classical regime at high energies, we find that quantum corrections to classical dynamics tend to decrease the Lyapunov exponents, which is essential for consistency with the Maldacena-Shenker-Stanford bound at low temperatures. The entanglement entropy is found to exhibit an expected “scrambling” behavior—rapid initial growth followed by saturation. At least at high temperatures the entanglement saturation time appears to be governed by classical Lyapunov exponents. Decay of quasinormal modes is found to be characterized by the shortest timescale of all. We also find that while the bosonic matrix model becomes nonchaotic in the low-temperature regime, for the full BFSS model with fermions the leading Lyapunov exponent, entanglement saturation time, and decay rate of quasinormal modes all remain finite and nonzero down to the lowest temperatures.
机译:我们在考虑和不考虑费米子的Banks-Fischler-Shenker-Susskind(BFSS)矩阵模型中,对Lyapunov指数,纠缠生成和准正态振铃进行了数值研究。我们使用最服从自洽运动方程的参数,根据最通用的高斯密度矩阵来近似实时动力学,从而将实时模拟的适用性扩展到经典极限之外。这些高斯密度矩阵的初始值经过优化,以尽可能接近系统的热平衡状态。因此,尝试在可计算的全息描述的低能态和高能的经典态之间架起桥梁,我们发现对经典动力学的量子校正趋向于降低Lyapunov指数,这对于与Maldacena-Shenker-Stanford保持一致至关重要在低温下绑定。发现纠缠熵表现出预期的“加扰”行为-快速的初始生长,然后达到饱和。至少在高温下,纠缠饱和时间似乎受经典的Lyapunov指数支配。发现准正常模式的衰减以所有时间尺度最短为特征。我们还发现,尽管玻色子矩阵模型在低温状态下变得非混沌,但对于具有费米子的完整BFSS模型,在最低温度下,领先的Lyapunov指数,纠缠饱和时间和准法向模的衰减率均保持有限且非零。 。

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