Fluctuation theorems impose constraints on possible work extraction probabilities in thermodynamical processes. These constraints are stronger than the usual second law, which is concerned only with average values. Here, we show that such constraints, expressed in the form of the Jarzysnki equality, can be bypassed if one allows for the use of catalystsadditional degrees of freedom that may become correlated with the system from which work is extracted, but whose reduced state remains unchanged so that they can be re-used. This violation can be achieved both for small systems but also for macroscopic many-body systems, and leads to positive work extraction per particle with finite probability from macroscopic states in equilibrium. In addition to studying such violations for a single system, we also discuss the scenario in which many parties use the same catalyst to induce local transitions. We show that there exist catalytic processes that lead to highly correlated work distributions, expected to have implications for stochastic and quantum thermodynamics.Definition 1 (No macroscopic work). Given a sequence of N -particle systems initially at thermal equilibrium with inverse temperature β and channels C (implicitly depending on N ), we say that the processes represented by C fulfill the no macroscopic work (NMW) condition if the probability of an event extracting work per particle larger or equal than is arbitrarily small as N → ∞,As is clear from the above, channels that satisfy the JE, such as unitary channels, also satisfy NMW and Av-SL. We now turn to investigate violations of JE and NMW for non-unitary channels.
Violations of NMW and JEThe first main result of this work is to introduce a physically motivated family of channels C that violates both Accepted in Quantum 2020-02-06, click title to verify. Published under CC-BY 4.0.