We study slow diffusion processes of orbits through thin chaotic layer
s of 2m (m greater-than-or-equal-to 2)-dimensional symplectic maps (of
ten referred to as Arnol'd diffusion) on a 4-dimensional mapping model
of accelerator dynamics. Using a method proposed by Chirikov, we comp
ute diffusion rates of vertical displacements, \y(n)\, near the flat b
eam case, when the horizontal motion occurs within a thin chaotic laye
r of the corresponding 2-dimensional x(n), x(n+1) map. Our computation
distinguishes between regions of diffusive and quasiperiodic motion,
in which the respective rates are found to differ by 10-12 orders of m
agnitude for N = 10(8) iterations. For diffusion, \y(n)\ grows on the
average with n (n less-than-or-equal-to 10(8)), with a rate D(R) is-pr
oportional-to exp(aR) (a > 0, R2 = y0(2) + y1(2)), which gives accurat
e estimates of escape times N(esc) is-proportional-to D-1. Modelling s
ynchrotron oscillations by a periodic modulation on the ''betratron''
frequencies, we find that diffusion rates increase significantly and r
apid escape occurs above certain thresholds in the epsilon, OMEGA para
meter values, epsilon and OMEGA being the amplitude and frequency of t
he modulation respectively.