107 In this way the absolute values of the structure factors may be
found, not the phases (6. 8). The problem to find these phases is the
phase problem. The present article will treat the following topics. At
first the description of the ideal crystal will be given in Chap. B. The
underlying principles of this description are the concepts of reciprocal
lattice, FOURIER synthesis and sym- metry. The evaluation of the
intensity will then follow in Chap. C and D. Chap. E is concerned with
the phase problem and related topics. Though this article treats the
analysis of crystal structures, the fundamental concepts for other
structures will here be found too. But these topics, and the
experimental methods, will l find their place elsewhere . B. Description
of the crystalline state. I. Lattice theory. a) The direct lattice. 8.
Introduction. In Sect. 3, a description of the ideal crystal was given:
The space, occupied by a crystal, is divided into congruent
parallelepipeds, each with the same orientation. This parallelepiped is
defined by the three basic vectors, a, band c, drawn from an origin 0
(Fig. 2), and is called the primitive cell. This cell is filled with
atoms (or ions), and the same configuration of atoms is repeated in
space. It has been aptly called a three-dimensional wallpaper, as on a
wallpaper the same pattern is repeated again and again.