ABSTRACT
The interaction of X-rays of the wavelength of the order of lattice
constants and shorter ones, allow us to learn about the crystal
structure of materials. In this chapter, we will introduce the
principles of X-ray diffraction for the case of X-rays interacting
with an ideal crystal structure; we will limit our considerations
to the case when X-rays are scattered elastically. The scattering
of X-rays by electrons from the atoms will be treated within
the first-order Born approximation, and within the isolated-atom
approximation (each atom contributes separately to the electron
density).