Let
τ=∣t−t′∣. Integrating the
equation for
x and using independence of the two
noises gives
R(τ)=C2τ+∫0τ∫0τf02e−α∣s−s′∣dsds′.
With the supplied
integral,
R(τ)=C2τ+α22f02(ατ−1+e−ατ).
For
ατ≪1, the active contribution is ballistic,
f02τ2+O(τ3), in
addition to the Brownian term. For
ατ≫1,
R(τ)=(C2+α2f02)τ−α22f02+o(1),
so the long-
time motion is diffusive with an enhanced
diffusion coefficient.