In previous work, a homogenized theory presenting effective enhanced d
iffusion coefficients on large scales and long times for a passive sca
lar diffusing in the presence of an incompressible, periodic, two-dime
nsional, steady fluid flow has been developed which predicts sensitive
mean wind dependence in the Peclet dependence of the enhanced diffusi
on matrix. Specifically, it has been rigorously demonstrated that the
enhanced diffusion coefficients possess a discontinuity on a dense set
of mean wind directions in the limit of large Peclet number. Addition
ally, at finite Peclet number, the enhanced diffusivities have been sh
own numerically to admit complex Peclet dependence sensitively depende
nt upon the mean wind direction. Here, we demonstrate that this renorm
alized, complex, finite Peclet scaling behavior is quantitatively obse
rvable in finite time using highly resolved, and carefully benchmarked
Monte Carlo simulations of the underlying stochastic process through
comparison of the mean-squared particle displacement with the renormal
ized diffusion coefficients, and further exhibit striking agreement wi
th the predictions of homogenization theory including sensitive mean w
ind dependence.