2015
DOI: 10.1088/1742-6596/638/1/012001
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Nonequilibrium Response and Frenesy

Abstract: We present examples of how time-symmetric kinetic factors contribute to the response either in nonlinear order around equilibrium or in linear order around nonequilibrium. The phenomenology we associate to that so called frenetic contribution are negative differential conductivity, changes in the Einstein relation between friction and noise, and population inversion.

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Cited by 34 publications
(49 citation statements)
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“…In recent years, however, it has often been emphasized that in true nonequilibrium regimes the Boltzmann-Clausius correspondence between heat and degeneracy, or between thermodynamic potential and fluctuations gets broken. From second order onward in any driving, the nonequilibrium statistics is described dynamically both by a dissipative, time-antisymmetric quantity (entropy production) ánd by kinetic time-symmetric estimators, sometimes called dynamical activity [31][32][33], traffic [63], or frenesy [37,39] (see also [40]).…”
Section: Discussion On Nondissipative Effectsmentioning
confidence: 99%
See 1 more Smart Citation
“…In recent years, however, it has often been emphasized that in true nonequilibrium regimes the Boltzmann-Clausius correspondence between heat and degeneracy, or between thermodynamic potential and fluctuations gets broken. From second order onward in any driving, the nonequilibrium statistics is described dynamically both by a dissipative, time-antisymmetric quantity (entropy production) ánd by kinetic time-symmetric estimators, sometimes called dynamical activity [31][32][33], traffic [63], or frenesy [37,39] (see also [40]).…”
Section: Discussion On Nondissipative Effectsmentioning
confidence: 99%
“…the blowtorch theorem of Landauer [29,30]. A steady nonequilibrium condition for an open system is not only characterized by dissipation, but also by kinetic aspects that quantify the activity in the system and that are nondissipative by definition [16,29,[31][32][33][35][36][37][38][39][40][41][42][43][44][45].…”
Section: Introductionmentioning
confidence: 99%
“…Note, however, that there is not a univocal prescription for the choice of W h through the function M 36,37 . For a general discussion of different symmetric factors in the transition rates, see for instance 38 , or 39,40 in the context of lattice gas models. For simplicity, here we take M = 0.…”
Section: E Other Forms Of Non-equilibrium Fdrmentioning
confidence: 99%
“…The nonequilibrium version of the heat capacity provides a simple demonstration of the fact that in general one cannot expect to predict the response of the energy to thermal variations just from the unperturbed correlations between energy and fluctuating heat flows, as one would do by using the standard fluctuation-dissipation theorem for equilibrium systems. Also non-dissipative aspects play a crucial role: The response includes correlations between the observable and the so-called frenesy of the system [3,4], which is a measure of how frantically the system wanders about in phase space. Eventually our example of generalised heat capacity should help understanding how to construct a theory for steady state thermodynamics.…”
Section: Resultsmentioning
confidence: 99%
“…Out of equilibrium, in contrast, there are multiple linear response theories [2][3][4], some based on the manipulation of the density of states [5][6][7][8][9], some on dynamical systems techniques for evolving observables [10][11][12], and some on a pathweight approach for stochastic systems [13][14][15][16][17]. The latter has revealed that entropy production is not sufficient for understanding the linear response of nonequilibrium systems.…”
Section: Introductionmentioning
confidence: 99%