2008
DOI: 10.1140/epjst/e2008-00688-8
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Controllable 3D atomic Brownian motor in optical lattices

Abstract: Abstract. We study a Brownian motor, based on cold atoms in optical lattices, where atomic motion can be induced in a controlled manner in an arbitrary direction, by rectification of isotropic random fluctuations. In contrast with ratchet mechanisms, our Brownian motor operates in a potential that is spatially and temporally symmetric, in apparent contradiction to the Curie principle. Simulations, based on the Fokker-Planck equation, allow us to gain knowledge on the qualitative behaviour of our Brownian motor… Show more

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Cited by 4 publications
(6 citation statements)
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References 38 publications
(60 reference statements)
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“…The measured periodicity of the temperature also confirms that the diabatic potentials are the relevant potentials in the system, as shown in [14]. The two potentials in the classical simulations are therefore chosen as the two lowest diabatic potentials of the two state-dependent potentials of the DOL used in the experiment [17]. The simulation qualitatively reproduces the main features of our BM although it is based on a classical model.…”
supporting
confidence: 64%
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“…The measured periodicity of the temperature also confirms that the diabatic potentials are the relevant potentials in the system, as shown in [14]. The two potentials in the classical simulations are therefore chosen as the two lowest diabatic potentials of the two state-dependent potentials of the DOL used in the experiment [17]. The simulation qualitatively reproduces the main features of our BM although it is based on a classical model.…”
supporting
confidence: 64%
“…To qualitatively understand the induced drift dependence on the relative spatial phase, a simple classical model is used [17,18], see figure 1. Consider a classical Brownian particle situated in either of two symmetric and periodic potentials (U A and U B ), coupled with unequal transfer rates (γ A→B and γ B→A ).…”
mentioning
confidence: 99%
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“…Compared to the simulations in figure 12, the experimental results clearly deviate around ϕ = 0 and 2π both in x and z. This was also noticed in simulations using diabatic potential curves [31], which prompted us to use adiabatic curves in the present study. It is now clear that the discrepancy is not due to the shape of the potential, which calls for simulations where a more realistic model is used to approach the physical system at hand.…”
Section: Numerical Simulationsmentioning
confidence: 53%
“…We show in figure 3 the dependence of the average transport velocity on the relative spatial phase for the model described above with Γ 1→2 = 10Γ 2→1 = 1. We point out that it is this case (unequal transfer rates and random transfer times) that was assumed to most closely resemble the experimental implementation with cold caesium atoms [18,19,20,21], and was thus the only case studied theoretically in previous work [17,19,20,25].…”
Section: Directed Transport With Asymmetric Transfer Ratesmentioning
confidence: 93%