We consider lensing by a plasma whose electron density takes the form of a Gaussian random field with a Kolmogorov power spectrum: in the thin lens approximation, the lens is effectively two-dimensional and the power spectrum \(P(k)\propto k^{-{5\over 3}}\). This is a good model for twinkling produced by a turbulent medium.
The following picture shows a realization of the lens:
We calculate the intensity pattern produced by this lens, comprising an intricate caustic network with diffraction fringes:
We also consider a 2d Gaussian random field with a power spectrum \(P(k)\propto k^{-1}\):
The intensity pattern for this case are shown below, again for various lens strengths.