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In this paper, exact continuum equations are derived to the classical many-body system in the hydrodynamic limit without the utilisation of statistical mechanics. It is shown that the resulting equations are universal for a class of pair potentials, and, unlike in statistical mechanics based coarse-grained models, the momentum density field carries the temperature. Evidence for the presence of pseudo time-irreversible equilibration, heat and momentum transport is provided by analysing numerical solutions of the dynamical equations. The numerical solutions further indicate the presence of non-diffusional relaxation of the macroscopic order, which raises questions about the completeness of the classical many-body dynamics in regards of the second law of thermodynamics.
We study synchronisation between periodically driven, interacting classical spins undergoing a Hamiltonian dynamics. In the thermodynamic limit there is a transition between a regime where all the spins oscillate synchronously for an infinite time wi
We study the statistics of the work done, the fluctuation relations and the irreversible entropy production in a quantum many-body system subject to the sudden quench of a control parameter. By treating the quench as a thermodynamic transformation we
We introduce a semi-classical limit for many-body localization in the absence of global symmetries. Microscopically, this limit is realized by disordered Floquet circuits composed of Clifford gates. In $d=1$, the resulting dynamics are always many-bo
We present a semiclassical treatment of one-dimensional many-body quantum systems in equilibrium, where quantum corrections to the classical field approximation are systematically included by a renormalization of the classical field parameters. Our s
We study the dynamics of the statistics of the energy transferred across a point along a quantum chain which is prepared in the inhomogeneous initial state obtained by joining two identical semi-infinite parts thermalized at two different temperature