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Are you familiar with the H-theorem in classical statistical mechanics? There is a similar quantum H-theorem in BM. See https://en.wikipedia.org/wiki/Antony_Valentini#Quantum_equilibrium,_locality_and_uncertaintystevendaryl said:I don't see how that's true. The continuity equation only implies that if at time ##t_1##, the particle has a probability density of ##|\psi(x,t_1)|^2## of being at any position ##x##, then at a later time, this will continue to be true. But you have to assume that it's true initially. Isn't that what the issue of non-equilibrium is all about?