Low Lying Island

(math) Equivalence relation properties are just group axioms

The necessary definitions

We can talk about groups as a collection of symmetries but the formal way is to define them axiomatically. Here are the group axioms for a group G which has multiplication defined by gh for g,hG:

G1. (Closure): For every g,hG, ghG
G2. (Associativity): For every f,g,hG, we have f(gh)=(fg)h.
G3. (Identity): There exists an element eG such that for all gG, we have eg=ge=g.
G4. (Inverses): For each gG, there exists a g1G such that gg1=g1g=e.

We can show that the identity element is unique and the inverses are unique with relative ease. If you have seen groups, then I will take for granted that you have heard about equivalence relations. Given a set S, we can define an equivalence relation RS×S if the following conditions are satisfied:

R1. (Reflexivity): For all xS, (x,x)R
R2. (Symmetry): For all x,yS, if (x,y)R then (y,x)R.
R3. (Transitivity): For all x,y,zS, if (x,y)R and (y,z)R, then (x,z)R.

These two notions are more related than they look on the surface and we can formalize that they are the same using group actions. A group action is just a permutation of the elements of some set X arising by multiplication by a group element g. For instance, given the set {1,3,5,7}, the element g can add 2 to each element (modulo 7) and we have g·X={3,5,7,1}, which is just the previous set but shuffled. In fact, we can define the action on elements such as g·1=g(1)=3.

Using group actions

The main idea is to visualize the pair (x,y) as a process where we start at x and end at y. We denote this by g(x)=y. So every pair (x,y) is representing a g responsible for sending x to y. We call the set of such maps G for foreshadowing reasons.

If we want the set of pairs to be an equivalence relation, we need to have a g that maps all x's to themselves. So, we define e(x)=x for all xS, which is exactly the identity element of a group!

To have symmetry, for each g(x)=y, we must have an h which maps y back to x. This is the same as finding inverses within the group!

Transitivity puts up more of a fight as we wrangle the meaning out of it. It says that if I have (x,y) and (y,z) in R, then I can find (x,z) in R. This sounds a lot like closure, where I can multiply g and h and find gh in G. I claim that this is more than just closure, and transitivity actually encodes the action of multiplication itself using pairs. When two pairs of the form (x,y) and (y,z) are lined up together (using the AND operator, say), then multiplication can occur in the universe of groups. Transitivity even comes with associativity built in.

O ye of little faith

We have been a bit sloppy in our exposition above as (x,y) might not necessarily represent a unique element but rather a coset of elements. As an example, both the identity element and the transposition (24) in S5 preserve the set {1,3,5}. We can solve this by making sure our group action is faithful which means that if g(x)=h(x), then g=h. This is not necessary but helps with making the proofs simpler in this case.

We also need that each (x,y)R corresponds to some gG. This is somewhat like transitivity.

What is equality?

The question that stands before us before we do any proofs in this new language is what does g=h in the group universe correspond to in the proposition universe? I am not sure.

(to be continued...)