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Mathematical Methods for Physicists: A concise introduction - Site Map

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ELEMENTS OF GROUP THEORY<br />

Table 12.3.<br />

1 i 1 i E A B C<br />

1 1 i 1 i E E A B C<br />

i i 1 i 1 or A A B C E<br />

1 1 i 1 i B B C E A<br />

i i 1 i 1 C C E A B<br />

correspond respectively to the elements A 0 ; B 0 ; C 0 ; ... of G 0 , then the equation<br />

AB ˆ C implies that A 0 B 0 ˆ C 0 , etc., and vice versa. Two isomorphic groups<br />

have the same multiplication tables except <strong>for</strong> the labels attached to the group<br />

elements. Obviously, two isomorphic groups must have the same order.<br />

Groups that are isomorphic and so have the same multiplication table are the<br />

same or identical, from an abstract point of view. That is why the concept of<br />

isomorphism is a key concept to physicists. Diverse groups of operators that act<br />

on diverse sets of objects have the same multiplication table; there is only one<br />

abstract group. This is where the value and beauty of the group theoretical<br />

method lie; the same abstract algebraic results may be applied in making predictions<br />

about a wide variety physical objects.<br />

The isomorphism of groups is a special instance of homomorphism, which<br />

allows many-to-one correspondence.<br />

Example 12.9<br />

Consider the groups of Problems 12.2 and 12.4. The group G of Problem 12.2<br />

consists of the four elements E ˆ 1; A ˆ i; B ˆ1; C ˆi with ordinary multiplication<br />

as the rule of combination. The group multiplication table has the <strong>for</strong>m<br />

shown in Table 12.3. The group G 0 of Problem 12.4 consists of the following four<br />

elements, with matrix multiplication as the rule of combination<br />

<br />

E 0 ˆ 1 0<br />

0 1<br />

<br />

; A 0 ˆ<br />

<br />

0<br />

<br />

1<br />

1 0<br />

<br />

; B 0 ˆ 1 0<br />

0 1<br />

<br />

<br />

; C 0 ˆ 0 1<br />

1 0<br />

It is straight<strong>for</strong>ward to check that the group multiplication table of group G 0 has<br />

the <strong>for</strong>m of Table 12.4. Comparing Tables 12.3 and 12.4 we can see that they have<br />

precisely the same structure. The two groups are there<strong>for</strong>e isomorphic.<br />

<br />

:<br />

Example 12.10<br />

We stated earlier that diverse groups of operators that act on diverse sets of<br />

objects have the same multiplication table; there is only one abstract group. To<br />

illustrate this, we consider, <strong>for</strong> simplicity, an abstract group of order two, G 2 : that<br />

436

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