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- are supplied automatically; if all atoms are
- in special positions, some of those marked "Special:" may also apply. The
- conditions consist of a class of indices, such as "hkl", or "hhl", etc., and
- an equation such as "h+k+l=2n" (which is the condition for a body-centered or
- "I" lattice). The general form of these equations can be written as xh+yk+zl
- = wn (all coefficients are integers; wn means a number divisible by w, etc.).
- When adding absence conditions, you are required to choose the class of
- reflection, and to specify the coefficients x, y, z, and w, all of which are
- integers.
-
- You do not need to enter conditions which are given in the Tables in
- parentheses (these are implied by other conditions), nor do you need to
- permute the indices, as sometimes indicated in higher-symmetry groups by a
- partial circle with an arrow on it. For each set of symmetry-equivalent
- indices, it is only necessary to enter one class. For example, in trigonal
- crystals, the class "HHl" (h,h,-2h,l) will also apply to classes "2HHL" (-2h,
- h,h,l) and "H2HL" (h,-2h,h,l), and in hexagonal crystals the same class will
- also give three additional equivalent classes.
-
- ments.
-
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