17 - Finishing the Isomorphism Theorems

Theorem

Suppose KG (see Normal Subgroup) with π:GGK be the cannonical projection. Then:

  1. AB in G iff AB in GK=G
  2. AG implies AG. This becomes an iff when we have subgroups HG that contain K.
    Then assuming HG that contain K:
  3. AB then |B:A|=|B:A| (see Index (Groups))
  4. AB=AB
  5. AB=AB

Example

Consider D8:

If we alternatively look at K=r2={1,r2} then the left cosets of K in D8 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:

  1. 1=r2
  2. r=r3
  3. s=sr2
  4. sr=sr3
    which all are elements of D8K={1,r,s,sr}. But look! We can make some map:
    {1,s,sr2,r2}{1,s,sr2,r2}={1,s}
    namely, use π:D8D8K such that ggK=g. Then for each normal subgroup in the lattice (see the orange boxes in the picture of the lattice):
  5. H1={1,s,sr2,r2} has π(H1)=H1
  6. H2={1,r,r2,r3}{1,r,r2,r3}={1,r2}=H2.
  7. ... we can repeat with each normal subgroup, and we'll get π(Hi)=Hi.
  8. H3={1,sr3,r2,sr}{1,sr3,r2,sr}={1,sr}=H3
  9. But some of them became the other normal subgroups. Namely π({1,s})=H1
  10. π{1,sr2}=H4
  11. ...

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:

Recall what a Group Action is:

left action

A (left) action of Group G on set X consists of a set map:
σ:G×XX
Where (g,x)σ(g,x)=gx=gx such that:

  1. g1(g2x)=(g1g2)x for all g1,g2G,xX
  2. 1Gx=x for all xX

This definition may seem a bit loose, so mathematicians sometimes use another definition:

left action

A (left) action of G on X is a group Homomorphism (or Group Morphism) (map) σ:GSX={fXX|f is a bijection} (see Symmetric Group & Permutations)

We'll later see that these definitions are equivalent. However, let's first look at an example.

Often we'll use σg to represent how σ(g)=σg in the alternative definition above. Namely:
σg(x)=gx

An Example

  1. The trivial action of G on X is σ:GSX such that each g1. Namely gx=x for all gG,xX.
  2. The Dihedral Groups, like D8 for the symmetries of a square, acts on the set of vertices of that square (X={v1,v2,v3,v4} for simplicity, for example rv1=v2). Define σr=(v1 v2 v3 v4)(1 2 3 4). Then this is a group action, where σ:D8SXS4 where σr:r(1 2 3 4).

D8 can also act on the set Y={d1,d2}, the diagonals of the square:

Here σr=(d1 d2)(1 2). Here D8SYS2.

  1. One action of the group onto itself is left multiplication by the group operation:
    gg=gg
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 gG such that gx=1G for all xX? See the answer on Trivial Group Action.

We can ask two questions, for each xX :

  1. We have the Orbit of x, denoted Ox={gx|gG}, which is just the outputs of all g's applied to some x.
  2. We have the Stabilizers of x denoted Gx={gG|gx=x}.

We can ask ourselves a theorem:

Theorem

When G acts on a set X, for each xX there's a bijection between the Orbit of x and the cosets of the Stabilizers of x, denoted Gx, in G:
OxGGx
Thus |Ox|=|G:Gx| (see Index (Groups)). This map is done by gxgGx.

The idea here is that the 25 The Lattice of Subgroups of a Group are themselves vertices of, say, a Dihedral Groups, which themselves can be analyzed! The orbits here let us get to that point.

Proof

Define the set map f:OxGGx by f(gx)gGx.

First, is f well-defined (since we are not mapping from a quotient group)? Suppose g1x=g2x for g1,g2G and xX. Then:
g1x=g2xg21(g1x)=x(g21g1)x=xg21g1Gxg1Gx=g2Gxf(g1x)=f(g2x)
Next, is f surjective? Take any gGx in GGx. Then gxOx and f(gx)=gGx.

Is f injective? Suppose g1x=g2xOx. Then:
f(g1x)=f(g2x)g1x=g2x
Thus this is a valid Isomorphism!