2021
DOI: 10.1103/physreve.103.032146
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Equilibrium free-energy differences from a linear nonequilibrium equality

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Cited by 12 publications
(7 citation statements)
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“…A. Heat engines SST have been employed in the last decade to design irreversible heat-engines [27,56,71,76,80,82,101,[153][154][155][156][157][158][159][160][161][162][163][164][165][166]. Loosely speaking, these heat engines can be considered as the mesoscopic counterparts of the classical, macroscopic, heat engines, in which the branches of the corresponding cycle last for a finite time.…”
Section: Applications: Heat Engines and Beyondmentioning
confidence: 99%
“…A. Heat engines SST have been employed in the last decade to design irreversible heat-engines [27,56,71,76,80,82,101,[153][154][155][156][157][158][159][160][161][162][163][164][165][166]. Loosely speaking, these heat engines can be considered as the mesoscopic counterparts of the classical, macroscopic, heat engines, in which the branches of the corresponding cycle last for a finite time.…”
Section: Applications: Heat Engines and Beyondmentioning
confidence: 99%
“…The Brownian particle is coupled to a heat bath with constant temperature T . To realize finite-time isothermal transitions between two equilibrium states with same temperature, Li et al [34,35] proposed a framework of shortcuts to isothermality by introducing an auxiliary potential U a (x, p, t) so that the distribution function of the system always maintains the following canonical form ρ = e βF (λ)−βHo(x,p,λ) ,…”
Section: A Shortcuts To Isothermalitymentioning
confidence: 99%
“…Their approach consists of two steps: determining the driving potential in an extremely slow time evolution and then rescaling the time variable so that the Kramers equation works for finite-time regions. A more straightforward approach is the shortcut to isothermality [34,35] which is the correspondence of quasi-static isothermal process in finite-time thermodynamics. The calculations of work and heat are tractable in shortcuts to isothermality.…”
Section: Introductionmentioning
confidence: 99%
“…( 19) represents an ensemble average over trajectories starting from an arbitrary initial distribution ρ(Γ, 0), but with driving protocols designed according to the strategy of shortcuts to isothermality. The third relation establishes an equality between the free energy difference and the mean work performed by the original Hamiltonian H o [34,93],…”
mentioning
confidence: 99%