2000
DOI: 10.1103/physrevlett.84.2358
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Directed Current due to Broken Time-Space Symmetry

Abstract: We consider the classical dynamics of a particle in a one-dimensional space-periodic potential U(X) = U(X+2pi) under the influence of a time-periodic space-homogeneous external field E(t) = E(t+T). If E(t) is neither a symmetric function of t nor antisymmetric under time shifts E(t+/-T/2) not equal-E(t), an ensemble of trajectories with zero current at t = 0 yields a nonzero finite current as t-->infinity. We explain this effect using symmetry considerations and perturbation theory. Finally we add dissipation … Show more

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Cited by 365 publications
(570 citation statements)
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“…Owing to the complexity of the dynamics, for example the simultaneous presence of periodic and chaotic attractors, there is a need for proper choice of initial conditions and ensemble averaging over them to obtain realistic averages [14,19,29]. This fact has been exemplified in an (zero mean) ac modulated periodic Hamiltonian system [31].…”
Section: Introductionmentioning
confidence: 99%
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“…Owing to the complexity of the dynamics, for example the simultaneous presence of periodic and chaotic attractors, there is a need for proper choice of initial conditions and ensemble averaging over them to obtain realistic averages [14,19,29]. This fact has been exemplified in an (zero mean) ac modulated periodic Hamiltonian system [31].…”
Section: Introductionmentioning
confidence: 99%
“…[16], has also contributed significantly to the understanding of the subject. These deterministic ratchets, unaided by noise, are shown to yield current in overdamped [17,18], underdamped [14,16,19,20,21,22,23,24,25,27,28], as well as in Hamiltonian [29,30,31] periodic potential systems, and also in overdamped quenched disordered [32,34] systems. In these systems net current results, without the presence of applied nonzero average forcing or asymmetric fluctuations, due to the presence of various regular transporting or chaotic attractors depending on the initial conditions for given system parameter values.…”
Section: Introductionmentioning
confidence: 99%
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“…For e 2 = 0 and any value of the phase one could in principle observe a ratchet e ect in x, due to the breaking of the temporal symmetry f x (t + T=2) = −f x (t) [41]. Note, however, that in the underdamped limit b → 0 one has to deal also with the symmetry f x (−t + T=2) = f x (t), and the condition, = 0; , may be required for inertial systems with very low friction values.…”
Section: Onset Of Directed Transport Under Crossed ÿEldsmentioning
confidence: 99%