2011
DOI: 10.1103/physreve.83.051120
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Brownian motor with competing spatial and temporal asymmetry of potential energy

Abstract: A Brownian motor is considered which operates due to asymmetric dichotomic fluctuations of the spatially periodic asymmetric potential energy. As shown, the motion direction and stopping points of this motor are dictated by the competition between the spatial and temporal asymmetry of the potential energy (or solely by temporal asymmetry in the case that the potential energy sign fluctuates). For an asymmetric sawtooth potential, the Brownian-particle average velocity is calculated numerically as a function of… Show more

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Cited by 38 publications
(31 citation statements)
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“…For the case of Gaussian noise (i.e., α = 2), the effect was previously reported in Ref. [15]. In that work, the emergence of a current for a system that switches between two symmetric potentials at equal rates has been linked to the fact that the maxima and minima of both potentials are shifted relatively to each other.…”
Section: A Switching Between Two Potentialssupporting
confidence: 56%
See 1 more Smart Citation
“…For the case of Gaussian noise (i.e., α = 2), the effect was previously reported in Ref. [15]. In that work, the emergence of a current for a system that switches between two symmetric potentials at equal rates has been linked to the fact that the maxima and minima of both potentials are shifted relatively to each other.…”
Section: A Switching Between Two Potentialssupporting
confidence: 56%
“…In different contexts, the emergence of a current when two potentials are randomly switched, in the presence of Gaussian noise, has been associated to a shift in the position of the minima [15] or to a difference in potential depth [16]. However, it is easy to see that none of these conditions is necessary to produce a current.…”
Section: A Switching Between Two Potentialsmentioning
confidence: 99%
“…The adiabaticity condition implies that (i) transitions from V a (x) to V b (x) and vice versa are fast, and (ii) the particle residence times in states a and b, τ a and τ b , are large as compared to all characteristic times of the system. With these conditions satisfied, the solution for the drift velocity is known [13,21]:…”
Section: Symmetry Propertiesmentioning
confidence: 99%
“…Note that even if the potentials V a (x) and V b (x) alone are symmetric, their average, u(x), can be asymmetric, which results in a nonzero drift velocity (a simple example is given in Ref. [21]). On the other hand, both V a (x) and V b (x) can be asymmetric, but nevertheless A = 0 as this occurs in the case where…”
Section: Symmetry Propertiesmentioning
confidence: 99%
“…Two main paradigms are recognized in this concept: flashing ratchets [16][17][18] in which transported particles are exposed to a time-fluctuating binding potential along their periodic track, and rocking ratchets [19][20][21] in which the particles move in an asymmetric periodic potential under the action of a spatially uniform time-dependent zero-mean force. The properties of the two ratchet types essentially differ in the adiabatic limit and are characterized by the various mechanisms of current reversal [22,23].…”
Section: Introductionmentioning
confidence: 99%