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arXiv:1002.3932 · Physical Review B

Classical and quantum regimes of the inhomogeneous Dicke model and its Ehrenfest time

Oleksandr Tsyplyatyev, Daniel Loss

Published Jul 27, 2010• 18 citations
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Abstract

We show that in the few-excitation regime, the classical and quantum time evolution of the inhomogeneous Dicke model for $N$ two-level systems coupled to a single boson mode agree for $N⪢1$. In the presence of a single excitation only, the leading term in an $1/N$ expansion of the classical equations of motion reproduces the result of the Schr\"odinger equation. For a small number of excitations, the numerical solutions of the classical and quantum problems become equal for $N$ sufficiently large. By solving the Schr\"odinger equation exactly for two excitations and a particular inhomogeneity, we obtain $1/N$ corrections which lead to a significant difference between the classical and quantum solutions at a new time scale which we identify as an Ehrenferst time, given by ${\ensuremath{\tau}}_{E}=\sqrt{N/⟨{g}^{2}⟩}$, where $\sqrt{⟨{g}^{2}⟩}$ is an effective coupling strength between the two-level systems and the boson.

DOI
10.1103/physrevb.82.024305

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We show that in the few-excitation regime, the classical and quantum time evolution of the inhomogeneous Dicke model for NNN two-level systems coupled to a single boson mode agree for N⪢1N⪢1N⪢1. In the presence of a single excitation only, the leading term in an 1/N1/N1/N expansion of the classical equations of motion reproduces the result of the Schr"odinger equation. For a small number of excitations, the numerical solutions of the classical and quantum problems become equal for NNN sufficiently large. By solving the Schr"odinger equation exactly for two excitations and a particular inhomogeneity, we obtain 1/N1/N1/N corrections which lead to a significant difference between the classical and quantum solutions at a new time scale which we identify as an Ehrenferst time, given by \ensuremathτE=N/⟨g2⟩{\ensuremath{\tau}}_{E}=\sqrt{N/⟨{g}^{2}⟩}\ensuremathτE​=N/⟨g2⟩​, where ⟨g2⟩\sqrt{⟨{g}^{2}⟩}⟨g2⟩​ is an effective coupling strength between the two-level systems and the boson.
Using the exact eigenstates of the inhomogeneous Dicke model obtained by numerically solving the Bethe equations, we study the decay of bosonic excitations due to the coupling of the mode to an ensemble of two-level (spin 1/21/21/2) systems. We compare the quantum time evolution of the bosonic mode population with the mean-field description which, for a few bosons, agree up to a relatively long Ehrenfest time. We demonstrate that additional excitations lead to a dramatic shortening of the period of validity of the mean-field analysis. However, even in the limit where the number of bosons equal the number of spins, the initial instability remains adequately described by the mean-field approach leading to a finite, albeit short, Ehrenfest time. Through finite size analysis we also present indications that the mean-field approach could still provide an adequate description for thermodynamically large systems even at long times. However, for mesoscopic systems one cannot expect it to capture the behavior beyond the initial decay stage in the limit of an extremely large number of excitations.
We study the time dynamics of a single boson coupled to a bath of two-level systems (spins 1/2) with different excitation energies, described by an inhomogeneous Dicke model. Analyzing the time-dependent Schr\"odinger equation exactly, we find that at resonance the boson decays in time to an oscillatory state with a finite amplitude characterized by a single Rabi frequency if the inhomogeneity is below a certain threshold. In the limit of small inhomogeneity, the decay is suppressed and exhibits a complex (mainly Gaussian-like) behavior, whereas the decay is complete and of exponential form in the opposite limit. For intermediate inhomogeneity, the boson decay is partial and governed by a combination of exponential and power laws.
The Tavis-Cummings model (the Dicke model treated in the rotating-wave approximation), describing many two-level systems coupled to a single bosonic mode, has been long known to show collective semiclassical oscillations when prepared in an inverted state, with all two-level systems excited and the bosonic mode is empty. This paper discusses how the quantum dynamics approaches this semiclassical result for large numbers of two-level systems, focusing on how the eigenvalues approach their semiclassical limit. The approach to the semiclassical result is found to be slow, scaling like a power of the logarithm of the system size. Considering also the effect of weak detuning between the two-level system and the bosonic field, quantum corrections are again found to decay slowly with system size, such that for a fixed detuning, the quantum effects of detuning are greater than the classical effect.
We consider an exactly solvable inhomogeneous Dicke model which describes an interaction between a disordered ensemble of two-level systems with single mode boson field. The existing method for evaluation of Richardson–Gaudin equations in the thermodynamical limit is extended to the case of Bethe equations in Dicke model. Using this extension, we present expressions both for the ground state and lowest excited states energies as well as leading-order finite-size corrections to these quantities for an arbitrary distribution of individual spin energies. We then evaluate these quantities for an equally-spaced distribution (constant density of states). In particular, we study evolution of the spectral gap and other related quantities. We also reveal regions on the phase diagram, where finite-size corrections are of particular importance.
We study two dispersive regimes of the Dicke model in the dynamics of N two-level atoms interacting with a bosonic mode for long interaction times. Firstly, we analyze the model for the regime in which the qubit frequencies are equal and smaller than the mode frequency, and for values of the coupling strength similar or larger than the mode frequency, namely, the deep strong coupling regime. Secondly, we address an interaction that is dependent on the photon number, where the coupling strength is comparable to the geometric mean of the qubit and mode frequencies. We show that the associated dynamics is analytically tractable and provide useful frameworks with which to analyze the system behavior. In the deep strong coupling regime, we unveil the structure of unexpected resonances for specific values of the coupling, present for N ≥ 2, and in the photon-number-dependent regime we demonstrate that all the nontrivial dynamical behavior occurs in the atomic degrees of freedom for a given Fock state. We verify these assertions with numerical simulations of the qubit population and photon-statistic dynamics.
Abstract In the present paper we show that the Hamiltonian describing the resonant interaction of N two-level systems with a single-mode electromagnetic quantum field in the Coulomb gauge can be diagonalized with a high degree of accuracy using a simple basis set of states. This allows one to find an analytical approximation for the eigenvectors and eigenvalues of the system, which interpolates the numerical solution in a broad range of the coupling constant values. For the first time, we show that the energy spectrum of Dicke model (DM) as a function of N (with N ≫ 1 ) satisfies the simple scaling relation. In addition, the introduced basis states provide a regular way of calculating the corrections and estimating the convergence to the exact numerical solution. Analytical approximations and numerical results describing the energy spectrum are valid for both quantum Rabi model ( N = 1) and DM for N ⩾ 2 atoms.