International
Tables for Crystallography Volume C Mathematical, physical and chemical tables Edited by E. Prince © International Union of Crystallography 2006 |
International Tables for Crystallography (2006). Vol. C. ch. 1.1, p. 3
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For certain lattice types, it is usual in crystallography to refer to a `conventional' crystallographic basis instead of a primitive basis a, b, c. In that case,
,
, and
with all their integral linear combinations are lattice vectors again, but there exist other lattice vectors
,
with at least two of the coefficients
,
,
being fractional.
Such a conventional basis defines a conventional or centred unit cell for a corresponding point lattice, the volume of which may be calculated by analogy with V by substituting
for a, b, and c in (1.1.1.1)
.
If m designates the number of centring lattice vectors t with ,
may be expressed as a multiple of the primitive unit-cell volume V:
With the aid of equations (1.1.1.2)
and (1.1.1.3)
, the reciprocal basis
may be derived from
. Again, each reciprocal-lattice vector
is an integral linear combination of the reciprocal basis vectors, but in contrast to the use of a primitive basis only certain triplets h, k, l refer to reciprocal-lattice vectors.
Equation (1.1.1.5) also relates
to
, the reciprocal cell volume referred to
. From this it follows that
Table 1.1.1.1 contains detailed information on `centred lattices' described with respect to conventional basis systems.
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As a direct lattice and its corresponding reciprocal lattice do not necessarily belong to the same type of Bravais lattices [IT A (2005, Section 8.2.5
)], the Bravais letter of
is given in the last column of Table 1.1.1.1
. Except for P lattices, a conventionally chosen basis for
coincides neither with a*, b*, c* nor with
. This third basis, however, is not used in crystallography. The designation of scattering vectors and the indexing of Bragg reflections usually refers to
.
If the differences with respect to the coefficients of direct- and reciprocal-lattice vectors are disregarded, all other relations discussed in Part 1 are equally true for primitive bases and for conventional bases.
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