A detailed analysis of a three-beam diffraction dispersion surface is perfo
rmed to study the forbidden wavefields of thick-crystal Bragg reflections.
From the asymptotic transition between two- and three-beam diffraction, it
is found that the excitation state of each wavefield can be accurately dete
rmined with the two-beam criterion. Consequently, Bragg-case three-beam dif
fraction from thick crystals is either a four-mode diffraction process for
the Bragg-Laue geometry or a two-mode process for the Bragg-Bragg geometry,
and the amplitudes of the excited wavefields can be completely determined
by the entrance boundary conditions. Based on this picture, the intrinsic m
echanisms underlying three-beam Bragg reflections are clearly illustrated.