This paper derives and analyzes exact, nonlocal Langevin equations
appropriate in a cosmological setting to describe the interaction of some
collective degree of freedom with a surrounding environment.'' Formally, these equations are much more general, involving as they do a more or less arbitrary system,‘’ characterized by some time-dependent potential, which is
coupled via a nonlinear, time-dependent interaction to a bath'' of oscillators with time-dependent frequencies. The analysis reveals that, even in a Markov limit, which can often be justified, the time dependences and nonlinearities can induce new and potentially significant effects, such as systematic and stochastic mass renormalizations and state-dependent memory’’
functions, aside from the standard friction'' of a heuristic Langevin description. One specific example is discussed in detail, namely the case of an inflaton field, characterized by a Landau-Ginsburg potential, that is coupled quadratically to a bath of scalar radiation.‘’ The principal conclusion
derived from this example is that nonlinearities and time-dependent couplings
do {\em not} preclude the possibility of deriving a fluctuation-dissipation
theorem, and do {\em not} change the form of the late-time steady state
solution for the system, but {\em can} significantly shorten the time scale for
the approach towards the steady state.

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