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Mathematical Methods for Physicists: A concise introduction - Site Map

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SOME SPECIAL GROUPS<br />

Figure 12.2.<br />

Some symmetry operations are equivalent. As shown in Fig. 12.2, a two-fold<br />

inversion axis is equivalent to a mirror plane perpendicular to the axis.<br />

There are two di€erent ways of looking at a rotation, as shown in Fig. 12.3.<br />

According to the so-called active view, the system (the body) undergoes a rotation<br />

through an angle , say, in the clockwise direction about the x 3 -axis. In the passive<br />

view, this is equivalent to a rotation of the coordinate system through the same<br />

angle but in the counterclockwise sense. The relation between the new and old<br />

coordinates of any point in the body is the same in both cases:<br />

x1 0 9<br />

ˆ x 1 cos ‡ x 2 sin ; >=<br />

x2 0 ˆx 1 sin ‡ x 2 cos ;<br />

…12:6†<br />

>;<br />

x3 0 ˆ x 3 ;<br />

where the prime quantities represent the new coordinates.<br />

A general rotation, re¯ection, or inversion can be represented by a linear<br />

trans<strong>for</strong>mation of the <strong>for</strong>m<br />

x1 0 9<br />

ˆ 11 x 1 ‡ 12 x 2 ‡ 13 x 3 ; >=<br />

x2 0 ˆ 21 x 1 ‡ 22 x 2 ‡ 23 x 3 ;<br />

…12:7†<br />

>;<br />

x3 0 ˆ 31 x 1 ‡ 32 x 2 ‡ 33 x 3 :<br />

Figure 12.3.<br />

(a) Active view of rotation; (b) passive view of rotation.<br />

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