零和非零温度下理想玻色极化子的猝灭动力学

Moritz Drescher, M. Salmhofer, T. Enss
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引用次数: 10

摘要

我们给出了在零和非零温度以及杂质-玻色子耦合的任意强度下,理想玻色-爱因斯坦凝聚体(我们称之为理想玻色极化子)中固定杂质的详细描述。我们精确地解出了时间演化,并且惊奇地发现,在这个更简单的设置中已经存在了许多已经预测到的真实BEC的特征,并且可以在其中解析地理解。得到了$T=0$时凝析波函数和$T>0$时单粒子密度矩阵时间演化的显式公式。对于负散射长度,即使动力学完全相干,系统也会发生热化。推导了Tan接触的时间演化和热值,并与最近的实验进行了比较。我们发现,与费米极化子相反,只要存在凝聚体,接触就不受统一性的限制。T=0处的动态重叠的显式公式使我们能够计算射频频谱,可以通过将其与一个玻色子和杂质的两体问题联系起来来详细理解。
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Quench Dynamics of the Ideal Bose Polaron at Zero and Nonzero Temperatures
We give a detailed account of a stationary impurity in an ideal Bose-Einstein condensate, which we call the ideal Bose polaron, at both zero and non-zero temperatures and arbitrary strength of the impurity-boson coupling. The time evolution is solved exactly and it is found that, surprisingly, many of the features that have been predicted for the real BEC are already present in this simpler setting and can be understood analytically therein. We obtain explicit formulae for the time evolution of the condensate wave function at $T=0$ and of the one-particle density matrix at $T>0$. For negative scattering length, the system is found to thermalize even though the dynamics are perfectly coherent. The time evolution and thermal values of the Tan contact are derived and compared to a recent experiment. We find that contrary to the Fermi polaron, the contact is not bounded at unitarity as long as a condensate exists. An explicit formula for the dynamical overlap at $T=0$ allows us to compute the rf spectrum which can be understood in detail by relating it to the two-body problem of one boson and the impurity.
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