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Experimental evidence of the failure of Jarzynski equality in active baths

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arxiv 1601.01123 v1 pith:KJYT6B7Q submitted 2016-01-06 cond-mat.soft

classification cond-mat.soft
keywords equalityjarzynskibathequilibriumactiveexperimentaldifferencefree-energy
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Most natural and engineered processes, such as biomolecular reactions, protein folding, and population dynamics, occur far from equilibrium and, therefore, cannot be treated within the framework of classical equilibrium thermodynamics. The Jarzynski equality holds the promise to calculate the free-energy difference between two states from the Boltzmann-weighted statistics of the irreversible work done along trajectories arbitrarily out of equilibrium. This equality is the subject of intense activity. However, the applicability of the Jarzynski equality to systems far from equilibrium such as living matter has not been investigated yet. We present an experimental test of the Jarzynski equality predictions on a paradigmatic physical model, i.e. a Brownian particle held in an optical potential, coupled either to a thermal bath or to an active bath. While in the thermal bath we find that the Jarzynski equality correctly retrieves the free-energy difference from nonequilibrium measurements, in the active bath the Jarzynski equality fails because of the presence of non-Boltzmann statistics. We corroborate our experimental findings with theoretical arguments and numerical simulations.

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Cited by 2 Pith papers

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  1. Entropy-production fluctuation theorem for a generalized Langevin particle in crossed electric and magnetic fields

    cond-mat.stat-mech 2025-12 conditional novelty 5.0 of 10

    For a generalized Langevin particle in crossed E and B fields, the total entropy production is Gaussian with variance equal to twice its mean, giving P(Δs)/P(−Δs)=e^{Δs}.

  2. Exact and variational identities for free energy differences in strongly coupled open systems

    cond-mat.stat-mech 2025-11 reject novelty 2.0 of 10

    The claimed exact fluctuation relations reduce to Hamiltonian-of-mean-force free-energy-perturbation identities; their trajectory forms require the final state to be exactly canonical, and the advertised variational/B...

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