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The basics of crystallography and diffraction (3rd Edition)

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5.3 Indexing lattice planes—Miller indices 133<br />

different point along OL—say Q—with coordinates 1 4 ,0, 1 2<br />

, we would have obtained<br />

the same result.<br />

Now consider the direction SN. To find its direction symbol the origin must be shifted<br />

from O to S. Proceeding as before (e.g. finding the coordinates <strong>of</strong> G with respect to the<br />

origin at S) gives the direction symbol [1¯10] (pronounced one bar-one oh), the bar or<br />

minus sign referring to a coordinate in the negative sense along the crystal axis.<br />

Directions in crystals are, <strong>of</strong> course, vectors, which may be expressed in terms <strong>of</strong><br />

components on the three unit cell edge or ‘base’ vectors a, b <strong>and</strong> c. In the above example<br />

the direction OL is written<br />

r 102 = 1a + 0b + 2c.<br />

<strong>The</strong> general symbol for a direction is [uvw] or, written as a vector,<br />

r uvw = ua + vb + wc.<br />

<strong>The</strong> direction symbols for the unit cell edge vectors a, b <strong>and</strong> c are [100], [010] <strong>and</strong><br />

[001], <strong>and</strong> very <strong>of</strong>ten these symbols are used in preference to the terms x-axis, y-axis<br />

<strong>and</strong> z-axis.<br />

5.3 Indexing lattice planes—Miller indices<br />

First, for reasons which will be apparent shortly, the lattice plane whose index is to be<br />

determined must not pass through the origin <strong>of</strong> the unit cell, or rather the origin must<br />

be shifted to a corner <strong>of</strong> the cell which does not lie in the plane. Consider the unit cell<br />

in Fig. 5.2 (identical to Fig. 5.1 but drawn separately to avoid confusion). We shall<br />

determine the index <strong>of</strong> the lattice plane which is shaded <strong>and</strong> outlined by the letters RMS.<br />

It is important first to realize that this plane extends indefinitely through the crystal; the<br />

shaded area is simply that portion <strong>of</strong> the plane that lies within the unit cell <strong>of</strong> Fig. 5.2.<br />

It is also important to realize that we are not just considering one plane but a whole<br />

family <strong>of</strong> identical, parallel planes passing through the crystal. <strong>The</strong> next plane ‘up’ in<br />

c<br />

z<br />

R<br />

P<br />

H<br />

y<br />

O<br />

b<br />

M<br />

S<br />

a<br />

G<br />

F<br />

x<br />

Fig. 5.2. Primitive unit cell (identical to Fig. 5.1), showing the first two planes, RMS <strong>and</strong> PGFH, in<br />

the family. <strong>The</strong>se planes are shaded within the confines <strong>of</strong> the unit cell.

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