Planckian dissipation bounds emerge as the requirement for classical hydrodynamics to stay valid at low temperature in quantum systems, via blurring from the quantum fluctuation-dissipation theorem.
[28], Mauger–Pottier derived iℏR ′′ BA(t) = 1 π CBA ∗pv Ω sinh(Ωt) ,(A8) CBA(t) =− iℏ π R′′ BA ∗pv Ω coth(Ωt) ,(A9) where∗denotes convolution
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Planckian dissipation from classical hydrodynamics
Planckian dissipation bounds emerge as the requirement for classical hydrodynamics to stay valid at low temperature in quantum systems, via blurring from the quantum fluctuation-dissipation theorem.