Consider an ``imperfect" crystal, where the nth atom is displaced
from its ideal position,
, by a random vector
.
We will look at the diffraction peak at around the reciprocal lattice vector
. Assume that
the displacement at site n is
, where a is the
average lattice spacing. Show that the
diffraction peak intensity will change little for small
, but
will disappear at larger
! What is the shape of the
envelope (peak height versus
)?
Laszlo Mihaly
Thu Oct 31 13:23:11 EST 1996