2014
DOI: 10.1088/1367-2630/16/9/095001
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Work statistics in stochastically driven systems

Abstract: We identify the conditions under which a stochastic driving that induces energy changes into a system coupled with a thermal bath can be treated as a work source. When these conditions are met, the work statistics satisfy the Crooks fluctuation theorem traditionally derived for deterministic drivings. We illustrate this fact by calculating and comparing the work statistics for a two-level system driven respectively by a stochastic and a deterministic piecewise constant protocol.

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Cited by 52 publications
(97 citation statements)
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“…When such small-scale machines are driven by external forces, like temperature or concentration gradient, shear flow, time-dependent external field, etc., observables such as work done, heat flow, power injection, entropy production, etc., become stochastic quantities [18][19][20][21][22][23][24][25][26][27][28][29][30]. The probability distributions of these quantities have richer information than their ensemble average values.…”
Section: Introductionmentioning
confidence: 99%
“…When such small-scale machines are driven by external forces, like temperature or concentration gradient, shear flow, time-dependent external field, etc., observables such as work done, heat flow, power injection, entropy production, etc., become stochastic quantities [18][19][20][21][22][23][24][25][26][27][28][29][30]. The probability distributions of these quantities have richer information than their ensemble average values.…”
Section: Introductionmentioning
confidence: 99%
“…This driving is symmetric under time-reversal (up to a time shift negligible in the long time limit) and the single reservoir version of this model was studied analytically in Refs. [20,21]. The work and heat CGF can also be calculated analytically for our machine as described in the Appendix.…”
Section: ν [H(t)] = ν [H(t)]/[2 Cosh β ν H(t)] But Arrhenius Rates ωmentioning
confidence: 99%
“…Changes in the control state leads to changes in the energies of the internal states and in the energy barriers between internal states. These changes can happen at fixed times for a deterministic protocol or at exponentially distributed waiting times for a stochastic protocol [11,12]. An internal current, i.e., net movement of the particle in the circle, in the clockwise direction can be induced by the external control in figure 2.…”
Section: Illustrative Examplementioning
confidence: 99%
“…The external protocol becomes unaffected by the dynamics of the internal system in the following limit [12]. The free energy difference is written as…”
Section: Limit Of Irreversible Controlmentioning
confidence: 99%