Solid State Chemistry and its Applications. Anthony R. West

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Solid State Chemistry and its Applications - Anthony R. West

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as shown in Table 1.30 for P ModifyingAbove 1 With bar. The general positions are listed first followed by the various special positions; for each, the first column gives the multiplicity, i.e. the number of equivalent positions. The second column is the so‐called Wyckoff notation in inverse alphabetical sequence; the logic behind this labelling scheme is that those positions at the bottom of the list have highest point symmetry and the symmetry may decrease on moving upwards through the list. The third column specifies the point symmetry of the positions. In this case, all the special positions coincide with a centre of symmetry whereas the general position, labelled as 2(i), has no point symmetry.

       1.18.5.2 Monoclinic C2

      Table 1.30 Coordinates and labelling of equivalent positions in space group P ModifyingAbove 1 With bar

Number of positions Wyckoff notation Point symmetry Coordinates of equivalent positions
2 I 1 xyz, x overbar y overbar z overbar
1 h ModifyingAbove 1 With bar ½, ½, ½
1 g ModifyingAbove 1 With bar 0, ½, ½
1 f ModifyingAbove 1 With bar ½, 0, ½
1 e ModifyingAbove 1 With bar ½, ½, 0
1 d ModifyingAbove 1 With bar ½, 0, 0
1 c ModifyingAbove 1 With bar 0, ½, 0
1 b ModifyingAbove 1 With bar 0, 0, ½
1 a ModifyingAbove 1 With bar 0, 0, 0

      The C‐centring in space group C2 means that if the Bravais lattice has a lattice point at the origin (with coordinates 0, 0, 0), it also has an equivalent lattice point in the middle of the side bounded by a and b, at ½, ½, 0. For any position x, y, z in this space group, there will, therefore, be an equivalent position at x + ½, y + ½, z. This C‐centring has no representation in the right‐hand diagram of Fig. 1.62 but can be seen in the left‐hand diagram; for example, positions 1 and 2 are related by the C‐centring.

      The main symmetry element present in space group C2 is a 2‐fold rotation axis parallel to b; it passes through the origin and is coincident with the y axis of the unit cell. The symbol for a 2‐fold rotation axis in the plane of the paper is an arrow. In this case, it is parallel to and coincident with y, passes through the origin x = 0, z = 0, and is shown by arrow d in the right‐hand diagram. The effect of the 2‐fold rotation axis on position 1, left‐hand diagram with coordinates x, y, z, is to generate the equivalent position shown as 3′, with coordinates −x, y, −z.

      Other symmetry elements are generated automatically by a combination of this 2‐fold rotation axis and the C‐centring. Thus, another 2‐fold rotation axis, e, parallel to b, is created which cuts the x axis at ½ and the z axis at 0; positions 1 and 3 are related by this 2‐fold axis, as are positions 3′ and 1‴, positions 4 and 2, etc.

      We also find that 2‐fold screw axes have been created automatically in this space group. A 2‐fold screw axis, symbol 21, involves a rotation component of 180o and a translation by ½ in the direction of the screw axis. Two 21 screw axes, f and g, are shown which are parallel to b, cut the x axis at one fourth comma three fourths and are in the plane of the unit cell projection at z = 0. Screw axes in the plane of the paper are represented as half‐arrows. Screw axis f relates positions 1, 4 and 1′ on an imaginary spiral that passes through the unit cell. The 21 screw axis is a combined translation and rotation operation. Thus, position 1 is translated halfway along y, retaining its x and z values, to the position shown as the dashed circle and then rotated by 180° about the axis parallel to y and at x = one fourth, z = 0, to arrive at position 4; it is important to recognise that the dashed circle is not an equivalent position but is drawn merely to show that two operations are involved in the screw axis. Positions 3′, 2, and 3″ are similarly related by the same screw axis.

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