We consider non-linear stochastic field equations such as the KPZ equation for deposition and the noise driven Navier-Stokes equation for hydrodynamics. We focus on the Fourier transform of the time dependent two point field correlation, $Phi_{bf{k}}(t)$. We employ a Lagrangian method aimed at obtaining the distribution function of the possible histories of the system in a way that fits naturally with our previous work on the static distribution. Our main result is a non-linear integro-differential equation for $Phi_{bf{k}}(t)$, which is derived from a Peierls-Boltzmann type transport equation for its Fourier transform in time $Phi_{bf{k}, omega}$. That transport equation is a natural extension of the steady state transport equation, we previously derived for $Phi_{bf{k}}(0)$. We find a new and remarkable result which applies to all the non-linear systems studied here. The long time decay of $Phi_{bf{k}}(t)$ is described by $Phi_{bf{k}}(t) sim exp(-a|{bf k}|t^{gamma})$, where $a$ is a constant and $gamma$ is system dependent.
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