  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
$\epsilon\gg<\epsilon>$ is shown to be stretched exponent $\ln{\cal
P}(\epsilon)\propto\epsilon^{1/3}$. At $\epsilon\ll<\epsilon>$, ${\cal
P}\propto 1/\sqrt{\epsilon}$.
