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Mathematical Methods for Physicists: A concise introduction - Site Map

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ELEMENTS OF GROUP THEORY<br />

The same set of all integers does not <strong>for</strong>m a group under multiplication. Why?<br />

Because the inverses of integers are not integers and so they are not members of<br />

the set.<br />

Example 12.3<br />

The set of all rational numbers (p=q, with q 6ˆ 0) <strong>for</strong>ms a continuous in®nite group<br />

under addition. It is an Abelian group, and we denote it by S 2 . The identity<br />

element is 0; and the inverse of a given element is its negative.<br />

Example 12.4<br />

The set of all complex numbers …z ˆ x ‡ iy† <strong>for</strong>ms an in®nite group under<br />

addition. It is an Abelian group and we denote it by S 3 . The identity element<br />

is 0; and the inverse of a given element is its negative (that is, z is the inverse<br />

of z).<br />

The set of elements in S 1 is a subset of elements in S 2 , and the set of elements in<br />

S 2 is a subset of elements in S 3 . Furthermore, each of these sets <strong>for</strong>ms a group<br />

under addition, thus S 1 is a subgroup of S 2 ,andS 2 a subgroup of S 3 . Obviously<br />

S 1 is also a subgroup of S 3 .<br />

Example 12.5<br />

The three matrices<br />

<br />

~A ˆ 1 0<br />

0 1<br />

<br />

; ~B ˆ<br />

<br />

0 1<br />

1 1<br />

<br />

; ~C ˆ<br />

1 1<br />

1 0<br />

<strong>for</strong>m an Abelian group of order three under matrix multiplication. The identity<br />

element is the unit matrix, E ˆ ~A. The inverse of a given matrix is the inverse<br />

matrix of the given matrix:<br />

<br />

~A 1 ˆ 1 0 <br />

<br />

<br />

ˆ ~A; ~B 1 1 1<br />

ˆ ˆ ~C; ~C 1 0 1<br />

ˆ<br />

ˆ ~B:<br />

0 1<br />

1 0<br />

1 1<br />

It is straight<strong>for</strong>ward to check that all the four group axioms are satis®ed. We<br />

leave this to the reader.<br />

Example 12.6<br />

The three permutation operations on three objects a; b; c<br />

‰1 23Š; ‰2 31Š; ‰3 12Š<br />

<strong>for</strong>m an Abelian group of order three with sequential per<strong>for</strong>mance as the law of<br />

combination.<br />

The operation [1 2 3] means we put the object a ®rst, object b second, and object<br />

c third. And two elements are multiplied by per<strong>for</strong>ming ®rst the operation on the<br />

432

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