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Mathematical Methods for Physicists: A concise introduction - Site Map

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ELEMENTS OF GROUP THEORY<br />

Table 12.6.<br />

~E ~A ~B<br />

~E ~E ~A ~B<br />

~A ~A ~B ~E<br />

B ~B ~E ~A<br />

axis is a threefold symmetry axis. There are three additional axes of symmetry in<br />

the xy plane: each corner and the geometric center O de®ning an axis; each of<br />

these is a twofold symmetry axis (Fig. 12.4). Now let us consider re¯ection operations.<br />

The following successive operations will bring the equilateral angle onto<br />

itself (that is, be invariant):<br />

~E the identity; triangle is left unchanged;<br />

~A triangle is rotated through 1208 clockwise;<br />

~B triangle is rotated through 2408 clockwise;<br />

~C triangle is re¯ected about axis OR (or the y-axis);<br />

~D triangle is re¯ected about axis OQ;<br />

~F triangle is re¯ected about axis OP.<br />

Now the re¯ection about axis OR is just a rotation of 1808 about axis OR, thus<br />

<br />

~C ˆ R OR …1808† ˆ 1 0 <br />

:<br />

0 1<br />

Next, we notice that re¯ection about axis OQ is equivalent to a rotation of 2408<br />

about the z-axis followed by a re¯ection of the x-axis (Fig. 12.5):<br />

<br />

~D ˆ R OQ …1808† ˆ ~C ~B ˆ 1 0 p ! p<br />

1=2 3 =2<br />

p<br />

0 1 <br />

<br />

1=2 <br />

3 =2<br />

ˆ p<br />

!:<br />

3 =2 1=2 <br />

<br />

3 =2 1=2<br />

Figure 12.4.<br />

448

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