International
Tables for
Crystallography
Volume C
Mathematical, physical and chemical tables
Edited by E. Prince

International Tables for Crystallography (2006). Vol. C. ch. 1.1, p. 3

Section 1.1.1.2. Non-primitive crystallographic bases

E. Kocha

a Institut für Mineralogie, Petrologie und Kristallographie, Universität Marburg, Hans-Meerwein-Strasse, D-35032 Marburg, Germany

1.1.1.2. Non-primitive crystallographic bases

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For certain lattice types, it is usual in crystallography to refer to a `conventional' crystallographic basis [{\bf a}_c,{\bf b}_c,{\bf c}_c] instead of a primitive basis a, b, c. In that case, [{\bf a}_c], [{\bf b}_c], and [{\bf c}_c] with all their integral linear combinations are lattice vectors again, but there exist other lattice vectors [{\bf t}\in{\bf L}], [{\bf t}=t_1{\bf a}_c+t_2{\bf b}_c+t_3{\bf c}_c,]with at least two of the coefficients [t_1], [t_2], [t_3] being fractional.

Such a conventional basis defines a conventional or centred unit cell for a corresponding point lattice, the volume [V_c] of which may be calculated by analogy with V by substituting [{\bf a}_c,{\bf b}_c,{\bf c}_c] for a, b, and c in (1.1.1.1)[link].

If m designates the number of centring lattice vectors t with [0\le t_1,t_2,t_3\lt1], [V_c] may be expressed as a multiple of the primitive unit-cell volume V: [V_c=mV.\eqno (1.1.1.10)]With the aid of equations (1.1.1.2)[link] and (1.1.1.3)[link], the reciprocal basis [{\bf a}^*_c,{\bf b}^*_c,{\bf c}^*_c] may be derived from [{\bf a}_c,{\bf b}_c,{\bf c}_c]. Again, each reciprocal-lattice vector [{\bf r}^*=h{\bf a}^*_c+k{\bf b}^*_c+l{\bf c}^*_c\in{\bf L}^*]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)[link] also relates [V_c] to [V^*_c], the reciprocal cell volume referred to [{\bf a}^*_c,{\bf b}^*_c,{\bf c}^*_c]. From this it follows that [V^*_c={1\over m}V^*.\eqno (1.1.1.11)]

Table 1.1.1.1[link] contains detailed information on `centred lattices' described with respect to conventional basis systems.

Table 1.1.1.1| top | pdf |
Direct and reciprocal lattices described with respect to conventional basis systems

Direct latticeReciprocal lattice
[{\bf a}_c, {\bf b}_c, {\bf c}_c][{\bf a}^*_c, {\bf b}^*_c, {\bf c}^*_c] 
Bravais letterCentring vectorsUnit-cell volume [V_c]Conditions for reciprocal-lattice vectors [h{\bf a}^*_c+k{\bf b}^*_c+l{\bf c}^*_c]Unit-cell volume [V^*_c]Bravais letter
A[{1\over2}{\bf b}_c+{1\over2}{\bf c}_c]2V[k+l=2n][{1\over2}V^*]A
B[{1\over2}{\bf a}_c+{1\over2}{\bf c}_c]2V[h+l=2n][{1\over2}V^*]B
C[{1\over2}{\bf a}_c+{1\over2}{\bf b}_c]2V[h+k=2n][{1\over2}V^*]C
I[{1\over2}{\bf a}_c+{1\over2}{\bf b}_c+{1\over2}{\bf c}_c]2V[h+k+l=2n][{1\over2}V^*]F
F[{1\over2}{\bf a}_c+{1\over2}{\bf b}_c,] [{1\over2}{\bf a}_c+{1\over2}{\bf c}_c,] [{1\over2}{\bf b}_c+{1\over2}{\bf c}_c]4V[h+k=2n,] [h+l=2n,] [k+l=2n][{1\over4}V^*]I
R[{1\over3}{\bf a}_c+{2\over3}{\bf b}_c+{2\over3}{\bf c}_c], [{2\over3}{\bf a}_c+{1\over3}{\bf b}_c+{1\over3}{\bf c}_c]3V[-h+k+l=3n][{1\over3}V^*]R

As a direct lattice and its corresponding reciprocal lattice do not necessarily belong to the same type of Bravais lattices [IT A (2005[link], Section 8.2.5[link] )], the Bravais letter of [{\bf L}^*] is given in the last column of Table 1.1.1.1[link]. Except for P lattices, a conventionally chosen basis for [{\bf L}^*] coincides neither with a*, b*, c* nor with [{\bf a}^*_c,{\bf b}^*_c,{\bf c}^*_c]. This third basis, however, is not used in crystallography. The designation of scattering vectors and the indexing of Bragg reflections usually refers to [{\bf a}^*_c,{\bf b}^*_c,{\bf c}^*_c].

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.

References

First citation International Tables for Crystallography (2005). Vol. A, Space-group symmetry, edited by Th. Hahn, 5th ed. Heidelberg: Springer.Google Scholar








































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