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Comparative quantum and semiclassical analysis of atom-field systems. I. Density of states and excited-state quantum phase transitions

机译:原子场系统的比较量子和半经典分析。一,态密度和激发态量子相变

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We study the nonintegrable Dicke model and its integrable approximation, the Tavis-Cummings model, as functions of both the coupling constant and the excitation energy. Excited-state quantum phase transitions (ESQPT) are found analyzing the density of states in the semiclassical limit and comparing it with numerical results for the quantum case in large Hilbert spaces, taking advantage of efficient methods recently developed. Two different ESQPTs are identified in both models, which are signaled as singularities in the semiclassical density of states; one static ESQPT occurs for any coupling, whereas a dynamic ESQPT is observed only in the superradiant phase. The role of the unstable fixed points of the Hamiltonian semiclassical flux in the occurrence of the ESQPTs is discussed and determined. Numerical evidence is provided that shows that the semiclassical results describe very well the tendency of the quantum energy spectrum for any coupling in both models. Therefore, the semiclassical density of states can be used to study the statistical properties of the fluctuation in the spectra, a study that is presented in a companion paper.
机译:我们研究了不可积Dicke模型及其可积近似Tavis-Cummings模型,它是耦合常数和激发能的函数。发现了激发态量子相变(ESQPT),它利用最近开发的有效方法,对半经典极限中的态密度进行了分析,并将其与大希尔伯特空间中量子情形的数值结果进行了比较。在两个模型中都标识了两个不同的ESQPT,用半经典状态密度中的奇异性表示。任何耦合都会产生一个静态ESQPT,而仅在超辐射阶段才观察到动态ESQPT。讨论并确定了哈密顿半经典通量的不稳定定点在ESQPTs发生中的作用。提供的数值证据表明,半经典结果很好地描述了两个模型中任何耦合的量子能谱趋势。因此,状态的半经典密度可用于研究光谱波动的统计特性,该研究将在随附的论文中进行介绍。

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