  We establish a connection between non-Markovian memory effects and
thermodynamical quantities such as work. We show how memory effects can be
interpreted as revivals of work that can be extracted from a quantum system. We
prove that non-Markovianity may allow an increase in the extractable work even
when the entropy of the system is increasing. Our results have important
implications both in quantum thermodynamics and in quantum information theory.
In the former context they pave the way to the understanding of concepts like
work in a non-Markovian open system scenario. In the latter context they lead
to interesting consequences for quantum state merging protocols in presence of
noise.
