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arXiv:1202.5174 · Physical Review Letters

Tuning the Mobility of a Driven Bose-Einstein Condensate via Diabatic Floquet Bands

Tobias Salger, Sebastian Kling, S. Denisov, Alexey V. Ponomarev, Peter Hänggi A, Martin Weitz

Published Mar 28, 2013• 24 citations
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Abstract

We study the response of ultracold atoms to a weak force in the presence of a temporally strongly modulated optical lattice potential. It is experimentally demonstrated that the strong ac driving allows for a tailoring of the mobility of a dilute atomic Bose-Einstein condensate with the atoms moving ballistically either along or against the direction of the applied force. Our results are in agreement with a theoretical analysis of the Floquet spectrum of a model system, thus revealing the existence of diabatic Floquet bands in the atoms' band spectra and highlighting their role in the nonequilibrium transport of the atoms.

DOI
10.1103/physrevlett.110.135302

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We study the response of ultracold atoms to a weak force in the presence of a temporally strongly modulated optical lattice potential. It is experimentally demonstrated that the strong ac driving allows for a tailoring of the mobility of a dilute atomic Bose-Einstein condensate with the atoms moving ballistically either along or against the direction of the applied force. Our results are in agreement with a theoretical analysis of the Floquet spectrum of a model system, thus revealing the existence of diabatic Floquet bands in the atoms' band spectra and highlighting their role in the nonequilibrium transport of the atoms.
The paradoxical response, when a system produces an output - current, flux or rotation - in the direction opposite to an applied bias or torque, seemingly contradicts Newton's second law. Nevertheless, such a response, termed absolute negative mobility, can occur in a system driven far out of thermal equilibrium. In earlier works, the presence of strong decoherence mechanisms was regarded as a prerequisite for negative mobility to appear. Here we report an experimental and theoretical study showing absolute negative mobility in a fully coherent quantum regime. Using a rubidium Bose-Einstein condensate loaded in a time-periodically modulated optical lattice, we observe a negative response from a coherent quantum system. The experimental results are explained in terms of eigenstates of a time-periodic Hamiltonian. Our findings open new possibilities for the control of quantum transport in the decoherence-free limit.
Coherent directed quantum transport of ultracold rubidium atoms in an optical realization of a quantum rocking ratchet is investigated experimentally. By changing parameters of the underlying periodic modulations we resolve transport resonances in the mean momentum of a dilute atomic Bose-Einstein condensate. These resonances are attributed to the avoided crossings between Floquet eigenstates which are widely separated on the energy scale. By increasing the amplitude of the drive we observe a theoretically predicted bifurcation of a single-peak resonance into a doublet. Our results prove the feasibility of fine experimental control over nonequlibrium, coherent quantum transport in ac-driven optical lattices
Periodically driven quantum systems are currently explored in view of realizing novel many-body phases of matter. This approach is particularly promising in gases of ultracold atoms, where sophisticated shaking protocols can be realized and interparticle interactions are well controlled. The combination of interactions and time-periodic driving, however, often leads to uncontrollable heating and instabilities, potentially preventing practical applications of Floquet engineering in large many-body quantum systems. In this work, we experimentally identify the existence of parametric instabilities in weakly interacting Bose-Einstein condensates in strongly driven optical lattices through momentum-resolved measurements, in line with theoretical predictions. Parametric instabilities can trigger the destruction of weakly interacting Bose-Einstein condensates through the rapid growth of collective excitations, in particular in systems with weak harmonic confinement transverse to the lattice axis. Understanding the onset of parametric instabilities in driven quantum matter is crucial for determining optimal conditions for the engineering of modulation-induced many-body systems.
The ratchet phenomenon is a means to get directed transport without net forces. Originally conceived to rectify stochastic motion and describe operational principles of biological motors, the ratchet effect can be used to achieve controllable coherent quantum transport. This transport is an ingredient of several perspective quantum devices including atomic chips. Here we examine coherent transport of ultra-cold atoms in a rocking quantum ratchet. This is realized by loading a rubidium atomic Bose-Einstein condensate into a periodic optical potential subjected to a biharmonic temporal drive. The achieved long-time coherence allows us to resolve resonance enhancement of the atom transport induced by avoided crossings in the Floquet spectrum of the system. By tuning the strength of the temporal modulations, we observe a bifurcation of a single resonance into a doublet. Our measurements reveal the role of interactions among Floquet eigenstates for quantum ratchet transport.
We exploit the variation of the atomic interaction in order to move ultracold atoms with attractive interaction across an ac-driven periodic lattice. By breaking relevant symmetries, a gathering of atoms is achieved. Accurate control of the gathered atoms' positions can be demonstrated via the control of the atomic localization process. The localization process is analyzed with the help of the nonlinear Floquet states where the Landau-Zener tunneling between states is observed and controlled. Transport effects in the presence of disorder are discussed.