Integrability, multifractality, and two-photon dynamics in disordered Tavis-Cummings models

Agnieszka Wierzchucka, Francesco Piazza, Pieter W. Claeys
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Abstract

The Tavis-Cummings model is a paradigmatic central-mode model where a set of two-level quantum emitters (spins) are coupled to a collective cavity mode. Here we study the eigenstate spectrum, its localization properties and the effect on dynamics, focusing on the two-excitation sector relevant for nonlinear photonics. These models admit two sources of disorder: in the coupling between the spins and the cavity and in the energy shifts of the individual spins. While this model was known to be exactly solvable in the limit of a homogeneous coupling and inhomogeneous energy shifts, we here establish the solvability in the opposite limit of a homogeneous energy shift and inhomogeneous coupling, presenting the exact solution and corresponding conserved quantities. We identify three different classes of eigenstates, exhibiting different degrees of multifractality and semilocalization closely tied to the integrable points, and study their stability to perturbations away from these solvable points. The dynamics of the cavity occupation number away from equilibrium, exhibiting boson bunching and a two-photon blockade, is explicitly related to the localization properties of the eigenstates and illustrates how these models support a collective spin description despite the presence of disorder.
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无序塔维斯-康明斯模型中的积分性、多折射性和双光子动力学
Tavis-Cummings 模型是一个典型的中心模式模型,其中一组两级量子发射器(自旋)耦合到一个集体空腔模式。在这里,我们研究了特征谱、其定位特性以及对动力学的影响,重点是与非线性光子学相关的双激发部门。这些模型包含两个无序源:一是自旋与腔体之间的耦合,二是单个自旋的能量移动。虽然已知该模型在同质耦合和非同质能量移动的极限下是可精确求解的,但我们在此确立了在同质能量移动和非同质耦合的相反极限下的可求解性,给出了精确解和相应的守恒量。我们确定了三类不同的特征状态,它们表现出不同程度的多折射性和半定位性,与可整点紧密相连,并研究了它们对远离这些可解点的扰动的稳定性。远离平衡状态的空穴占据数的动力学表现出玻色子束化和双光子封锁,这与特征状态的局域化特性明确相关,并说明了这些模型如何在存在无序的情况下支持集体自旋描述。
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