Under these considerations is called a -set. Notice that we are not requiring to be related to in any way. It is true that every group acts on every set by the trivial action ; however, group actions are more interesting if the set is somehow related to the group .
Let and . Then acts on by left multiplication. If and is the identity matrix, then . If and are invertible matrices, then since matrix multiplication is associative.
The elements of act on as functions. The permutation acts on vertex by sending it to vertex , on vertex by sending it to vertex , and so on. It is easy to see that the axioms of a group action are satisfied.
Let be a -set. Then -equivalence is an equivalence relation on .
Proof.
The relation is reflexive since . Suppose that for . Then there exists a such that . In this case ; hence, . To show that the relation is transitive, suppose that and . Then there must exist group elements and such that and . So , and is equivalent to .
If is a -set, then each partition of associated with -equivalence is called an orbit of under . We will denote the orbit that contains an element of by .
Now suppose that is a group acting on a set and let be an element of . The fixed point set of in , denoted by , is the set of all such that . We can also study the group elements that fix a given . This set is more than a subset of , it is a subgroup. This subgroup is called the stabilizer subgroup or isotropy subgroup of . We will denote the stabilizer subgroup of by .
Let be a group acting on a set and . The stabilizer group of ,, is a subgroup of .
Proof.
Clearly, since the identity fixes every element in the set . Let . Then and . So ; hence, the product of two elements in is also in . Finally, if , then . So is in .
We will denote the number of elements in the fixed point set of an element by and denote the number of elements in the orbit of by . The next theorem demonstrates the relationship between orbits of an element and the left cosets of in .
Let be a finite group and a finite -set. If , then .
Proof.
We know that is the number of left cosets of in by Lagrangeβs Theorem (Theorem 6.10). We will define a bijective map between the orbit of and the set of left cosets of in . Let . Then there exists a in such that . Define by . To show that is one-to-one, assume that . Then
,
where and . Since , there exists a such that ,
consequently, the map is one-to-one. Finally, we must show that the map is onto. Let be a left coset. If , then .