The backscatter cross section

for high-frequency irradiated turbulent dielectric media, many mean free paths

wide, is computed. The length

is the distance into the medium over which the mean electric field decreases in amplitude by a factor

. Previous calculations have always been restricted to

. It is found that

increases from the Born approximation

for medium width

to

for

, and the theory is valid as long as

, a significant improvement over the Born approximation, when the macroscale

is much larger than the wavelength

. The improvement is due to incorporation of the dominant effects of cumulative forward scattering in the local electric field in the medium. A rigorous and a heuristic derivation are given. The transitional behavior is discussed and a simple physical interpretation is given.