Abstract

The stabilizing effect of quantum fluctuations on the escape process and the relaxation dynamics from a quantum metastable state are investigated. Specifically, the quantum dynamics of a multilevel bistable system coupled to a bosonic Ohmic thermal bath in strong dissipation regime is analyzed. The study is performed by a non-perturbative method based on the real-time path integral approach of the Feynman-Vernon influence functional. We consider a strongly asymmetric double well potential with and without a monochromatic external driving, and with an out-of-equilibrium initial condition. In the absence of driving we observe a nonmonotonic behavior of the escape time from the metastable region, as a function both of the system-bath coupling coefficient and the temperature. This indicates a stabilizing effect of the quantum fluctuations. In the presence of driving our findings indicate that, as the coupling coefficient increases, the escape time, initially controlled by the external driving, shows resonant peaks and dips, becoming frequency-independent for higher values. Moreover, the escape time from the metastable state displays a nonmonotonic behavior as a function of the temperature, the frequency of the driving, and the thermal-bath coupling, which indicates the presence of a quantum noise enhanced stability phenomenon. Finally, we investigate the role of different spectral densities, both in sub-Ohmic and super-Ohmic dissipation regime and for different cutoff frequencies, on the relaxation dynamics from the quantum metastable state. The results obtained indicate that, in the crossover dynamical regime characterized by damped intrawell oscillations and incoherent tunneling, the spectral properties of the thermal bath influence non-trivially the short time behavior and the time scales of the relaxation dynamics from the metastable state.

Highlights

  • The interaction between environmental random fluctuations and the nonlinearity of real systems can give rise to new unexpected phenomena

  • In the absence of driving, we study the dissipative dynamics in a system consisting of a quantum particle moving along an asymmetric bistable potential, while discussing some results previously obtained within the context of the noise enhanced stability

  • We reviewed some results on the escape processes from quantum metastable states strongly interacting with an Ohmic thermal bath

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Summary

Introduction

The interaction between environmental random fluctuations and the nonlinearity of real systems can give rise to new unexpected phenomena. This issue can be faced by taking into account a quantum particle, initially prepared in a nonequilibrium state within a strongly asymmetric bistable potential, and studying the dynamics of the spatially localized states of this system This approach allows to observe that, as the damping increases, the relaxation process towards the stable (lower) well undergoes a modification: the population transfer, characterized by a metastable well temporarily populated, becomes a direct transfer to the stable state, due to the fact that higher damping values tend to suppress the tunnel effect in the dissipation dynamics [29,41]. This reduced Hilbert space allows to pass, by suitably transforming, to the discrete variable representation (DVR) [67]. The parameters γ and T are given in units of ω0 and hω0 /k B , respectively

The Influence Functional and the Discrete Variable Representation
Master Equation
Transient Dynamics in the Absence of Driving
Results
Driven Quantum Dissipative Dynamics
E E4 b a
High-Frequency Driving
Escape Time for the Driven System
Results and Discussion
Dissipative Dynamics in Sub-Ohmic and Super-Ohmic Regime
Conclusions
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