“…In the absence of external forces (at f ( R , t ) = 0), the noise term in the GLE as obtained from the projection operator obeys a so-called second fluctuation dissipation theorem (2FDT) 〈 Γ ( t 0 ) Γ ( t )〉 eq = k B T K ( t − t 0 ). The effect of including external forces in a GLE description, 36,39–41 non-stationary dynamics, 42,43 and stochastic microscopic dynamics 44,45 has also been discussed using first principle theory. Important conclusions from these studies are that the 2FDT is no longer generally valid in such cases: namely, in the presence of non-linear or stochastic interactions, 45,46 external forces, or general non-equilibrium settings.…”