  We consider the continuous-time random walk of a particle in a
two-dimensional self-affine quenched random potential of Hurst exponent $H>0$.
The corresponding master equation is studied via the strong disorder
renormalization procedure introduced in Ref. [C. Monthus and T. Garel, J. Phys.
A: Math. Theor. 41 (2008) 255002]. We present numerical results on the
statistics of the equilibrium time $t_{eq}$ over the disordered samples of a
given size $L \times L$ for $10 \leq L \leq 80$. We find an 'Infinite disorder
fixed point', where the equilibrium barrier $\Gamma_{eq} \equiv \ln t_{eq}$
scales as $\Gamma_{eq}=L^H u $ where $u$ is a random variable of order O(1).
This corresponds to a logarithmically-slow diffusion $ | \vec r(t) - \vec r(0)
| \sim (\ln t)^{1/H}$ for the position $\vec r(t)$ of the particle.
