2016
DOI: 10.1088/1742-5468/2016/09/093205
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Housekeeping entropy in continuous stochastic dynamics with odd-parity variables

Abstract: We investigate the decomposition of the total entropy production in continuous stochastic dynamics when there are odd-parity variables that change their signs under time reversal. The first component of the entropy production, which satisfies the fluctuation theorem, is associated with the usual excess heat that appears during transitions between stationary states. The remaining housekeeping part of the entropy production can be further split into two parts. We show that this decomposition can be achieved in i… Show more

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Cited by 17 publications
(27 citation statements)
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References 30 publications
(99 reference statements)
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“…In that case, the mirror symmetry follows from the DB only after assuming a certain condition for the multiplicative noise strengths. In general the two conditions remain independent [35]. The broken mirror symmetry manifests the existence of nonzero average current j rev x p in position space, as seen from Eq.…”
Section: Detailed Balancementioning
confidence: 99%
“…In that case, the mirror symmetry follows from the DB only after assuming a certain condition for the multiplicative noise strengths. In general the two conditions remain independent [35]. The broken mirror symmetry manifests the existence of nonzero average current j rev x p in position space, as seen from Eq.…”
Section: Detailed Balancementioning
confidence: 99%
“…For example, one may regard a magnetic field as an odd parameter, so change the sign of a magnetic field in the time-reverse dynamics [21,47]. On the other hand, one may keep the sign of the magnetic field for the irreversibility [48][49][50][51][52], where the † dynamics is identical to the original time-forward dynamics. Nonetheless, we will show later that the generalized TUR does not depend on the choice of odd parameters.…”
Section: Model and Generalized Turmentioning
confidence: 99%
“…Since this correction term do not obey an integral fluctuation theorem, we cannot give any bounds on the sign of its mean. Considering transitions between stationary states and taking revised microscopic reversibility (46) into account, we can obtain the relation…”
Section: B Revising Microscopic Reversibilitymentioning
confidence: 99%
“…Spinney and Ford [42][43][44] recently investigated systems with odd dynamical variables (such as momentum that changes its sign under time-reversal operation) and found that the total entropy production can be separated into three parts, with two of them satisfying the integral fluctuation theorem. Lee et al [45,46] modified the separation rule for the total entropy production put forward in [42][43][44] and endowed each part of the total entropy production with clear physical origins.…”
Section: Introductionmentioning
confidence: 99%