Intermittent dissipation of a passive scalar in turbulence

Probability density function (PDF) of passive scalar dissipation ${\cal P} (\epsilon)$ is found analytically in the limit of large Peclet and Prandtl numbers (Batchelor-Kraichnan regime) in two dimensions. The tail of PDF at $ϵ\gg <ϵ>$ is shown to be stretched exponent $\ln{\cal P}(\epsilon)\propto\epsilon^{1/3}$\mathrm{.}At$\epsilon\ll<\epsilon>$,${\cal P}\propto 1/\sqrt{\epsilon}$.