“…In particular, they correctly describe both the rechanneling process and the large transverse energy fluctuations at the upper under-barrier region ε ⊥ ∼ ε ⊥max , in which the diffusion equation looses its applicability. Monte Carlo approach have also demonstrated its efficiency in simulation of the new effects of channeling probability increase by the crystal cut [23], positive miscut influence of collimation [24] and other possibilities of the latter [25], multiple new radiation features in both crystal undulators [2,26,27] and bent crystals [28,29], the effects of planar channeling and quasichanneling oscillations in the deflection angle distribution of particles passed through a bent crystal [30] and many effects in the field of atomic strings [31,32,33,34,35,36,37]. However the main purpose of this paper was to demonstrate that despite all the achievements of Monte Carlo method, the diffusion equation approach, refined in present paper, can supplement the simulation results with the enlightening treatment of the collective statistical behavior of channeling particles, which can not be described by the sum of two exponents decaying with nuclear and electron dechanneling lengths.…”