If we alternatively look at then the left cosets of in are:
Notice we don't care which representative we use for each subgroup of cosets, so then we can use the bar notation to indicate a coset:
which all are elements of . But look! We can make some map:
namely, use such that . Then for each normal subgroup in the lattice (see the orange boxes in the picture of the lattice):
has
.
... we can repeat with each normal subgroup, and we'll get .
But some of them became the other normal subgroups. Namely
...
We can make a lattice for what becomes what, and what stays the same:
Which is the same lattice picture we had before, but only with the normal subgroups!
Back to Group Actions
We'll be looking at specific examples of Group Actions in, well, action! For each one we'll look at the mechanical actions to see how to get things like:
We'll later see that these definitions are equivalent. However, let's first look at an example.
Often we'll use to represent how in the alternative definition above. Namely:
An Example
The trivial action of on is such that each . Namely for all .
The Dihedral Groups, like for the symmetries of a square, acts on the set of vertices of that square ( for simplicity, for example ). Define . Then this is a group action, where where .
can also act on the set , the diagonals of the square:
Here . Here .
One action of the group onto itself is left multiplication by the group operation:
Note
Why left multiplication? Namely, it's because our definition is in terms of terms from the group being on the left.
Is there any group elements that keeps each element fixed? Namely is there some such that for all ? See the answer on Trivial Group Action.
We can ask two questions, for each :
We have the Orbit of , denoted , which is just the outputs of all 's applied to some .
When acts on a set , for each there's a bijection between the Orbit of and the cosets of the Stabilizers of , denoted , in :
Thus (see Index (Groups)). This map is done by .