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Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics

Suppression or enhancement of quantum tunneling by a nonlinear resonance induced in a driven double-well system

Ju-Yong Shin

Published Jul 1, 1996• 3 citations
Publisher

Abstract

The effect of a periodic driving force on coherent tunneling of a driven double square-well system, especially when its central potential barrier is very tall and very thin, is investigated. The suppression or enhancement of the tunneling of a wave packet properly chosen in the double-well system may be achieved by a judicious choice of the period of a driving force, i.e., by a particular choice of the generating condition of a nonlinear resonance exhibiting a desirable property. We analyze this mechanism by exploiting both the properties of a dynamical symmetry of the Hamiltonian and the localized properties of Floquet states induced by the nonlinear resonance. \textcopyright{} 1996 The American Physical Society.

DOI
10.1103/physreve.54.289

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The effect of a periodic driving force on coherent tunneling of a driven double square-well system, especially when its central potential barrier is very tall and very thin, is investigated. The suppression or enhancement of the tunneling of a wave packet properly chosen in the double-well system may be achieved by a judicious choice of the period of a driving force, i.e., by a particular choice of the generating condition of a nonlinear resonance exhibiting a desirable property. We analyze this mechanism by exploiting both the properties of a dynamical symmetry of the Hamiltonian and the localized properties of Floquet states induced by the nonlinear resonance. \textcopyright{} 1996 The American Physical Society.
The second-order perturbation theory in the framework of the Kramers-Henneberger oscillating frame representation of the Hamiltonian [H. A. Kramers, Quantum Mechanics (North-Holland, Amsterdam, 1956); W. C. Henneberger, Phys. Rev. Lett. 21, 838 (1968)] is used to study the tunneling process in a periodically driven double-well potential. The eigenstates of the Floquet Hamiltonian are efficiently approximated when a field frequency is larger than a classical frequency of the time-averaged Hamiltonian. The conditions for coherent enhancement and suppression of tunneling are obtained when the standard perturbation theory fails. It is shown that the enhancement and suppression of tunneling is due to field-induced coupling between states of a one-period averaged effective potential.
Quantum tunneling dynamics of a periodically driven symmetric double-well system is studied within the framework of the Floquet theory. The role that a dynamical symmetry of the system plays in connection with tunneling is analyzed. The analysis shows that, in order to fully describe tunneling exhibited by a system with a dynamical symmetry, one should look at wave functions at times corresponding to integral multiples of the period of the driving force plus one-half period. The analysis shows also that tunneling can be understood to occur as a result of the quantum revival, a phenomenon well known in quantum optics. \textcopyright{} 1996 The American Physical Society.
We show that a field of frequency omega combined with its second harmonic 2omega driving a double-well potential allows us to localize the wave packet by adiabatic passage, starting from the delocalized ground state. The relative phase of the fields allows us to choose the well of localization. We can suppress (and restore) the tunneling subsequently by switching on (and off) abruptly the fields at well-defined times. The mechanism relies on the fact that the dynamics is driven to an eigenstate of the Floquet Hamiltonian which is a localized state.
The phenomenon of tunneling is investigated for a symmetric double-well potential perturbed by a monochromatic driving force. The analysis is based on a numerical treatment of the quantum map that propagates the system over one period of the external force, and of the spectrum of its eigenphases (quasienergies). The variety in the quasienergy spectrum, such as exact and avoided crossings, leads to novel forms of coherent tunneling. In particular, for specific parameter values of the driving force, we find almost complete localization of the wave packet in one of the wells.
The quantum dynamics of a particle in a double-well potential under a monochromatic external driving force is computed by using a minimum-uncertainty Gaussian wave packet as an initial state. Irregular or regular time development of dynamical variables is obtained, depending on whether the initial wave packet is located in the classical chaotic sea or the regular region in phase space, respectively. Tunnelings between nonresonant islands and between resonant islands are obtained. Tunneling times between nonresonant islands decrease smoothly, in general, with the increase of the amplitude of the driving force, but tunneling times between resonant islands are more erratic.