Partial Orders Lattices and Some Subgroups

Partial Orders Lattices and Some Subgroups
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In this article we mostly talk about partial orders, and lattices, which are a special type of partial order. We tie it in with our discussions of subgroups before proving two distribution laws for lattices.

Definition (partial order)

A partial order is a relation between two elements of a set,S, usually written , which satisfies the following axioms

  1. xS, xx.
  2. x,yS, xy and yx implies that x=y.
  3. x,y,zS, xy and yz implies xz.

When writing out the partial order, we sometimes write it as an ordered pair (S,), writing out the set and the partial order symbol.

As the name suggests, partial orders are less strict than total orders, like among the rational numbers. For example, if we take Q×Q with the relation (x1,x2)(y1,y2) if and only if x1y1 and x2=y2, then this is a partial order. We can see that all of the axioms are satisfied by this order, but there are many ordered pairs which can’t be compared with each other. For example, (1,2) and (2,1) aren’t comparable as x2y2.

Consider a second example of ordered pairs of rationals where (x1,x2)(y1,y2) if and only if x1y1 and x2y2. Notice that with this partial order on Q×Q, that for any pair of elements x and y, we can find a z, such that xz and yz. To see this, let (x1,x2) and (y1,y2) be two ordered pairs of rational numbers. Then if we let z=(max(x1,y1),max(x2,y2)), we see that xz and yz as we wanted. Similarly, by taking z=(min(x1,y1),min(x2,y2)), we have zx and zy.

However, the first example we gave didn’t have this property. To see that, consider the example pair we gave above, x=(1,2) and y=(2,1). There is no z which can be comparable to both x and y, because in that case z2, the second component of z, would have to equal both 1 and 2.

This brings us to our next few definitions.

Definition (lattice)

Let (S,) be a partial order such that for any two elements, x and y S, there exists w,zS, such that wx, wy, xz and yz, then this partial order is said to be a lattice.

Definition (join)

Let (S,) be a lattice. Let x and yS, then the -least element zS, such that xz and yz is said to be their join. It is typically written as z=xy.

This is also called max(x,y), which I used earlier when constructing the max of two ordered pairs. Hopefully that wasn’t too confusing, though, since I was using it in its more common setting, where the order is the usual order on the rationals. It can also be called the supremum of the set {x,y}. We’ll define that more precisely later.

Definition (meet)

Let (S,) be a lattice. Let x and yS, then the -greatest element zS, such that zx and zy is said to be their meet. It is typically written as z=xy.

More precisely, xy=z, where u,xu and yu implies zu. The precise definition for is similar. It is sometimes called min(x,y).

Notice that and are functions which map every element of S×S to another element of S, whenever (S,) is a lattice. Now we prove that it’s associative.

Definition ( >= )

Let (S,) be a partial order. Then we define to be the relation such that xy, if and only if yx for all x, yS.

Hopefully that last definition didn’t confuse or surprise anyone.

Theorem ( v is associative):

Let x, y and z be elements of S. Let’s S, be a lattice. Then, (xy)z=x(yz).

Proof

Let s:=xy, and t:=yz. Also let a:=sz and b:=xt. Then we have

a=sz

b=xt

Then, by definition, we have az, sy, and as. By the transitivity of , we have ay. Therefore, by the definition of t, we have at. We also have sx, which means that applying transitivity again, ax. This means, that, by the definition of b, ab. A similar argument will show that ba, and thus a=b by partial order axiom 2.

QED

Theorem ( ^ is associative)

Let x, y and z be elements of S. Let’s S, be a lattice. Then, (xy)z=x(yz).

Proof

Very similar to the proof for .

Definition (bounded lattice)

Let (S,) be a lattice, such that there are two elements of S, which we’ll call 1 and 0, such that for all sS, s1 and 0s. Then (S,) is said to be a bounded lattice.

Theorem (subgroups form a bounded lattice)

Let G be a group and let G:={HG}, then (G,), where H1H2 is the usual subgroup relation, is a bounded lattice.

Proof

By the definition of subgroup, we know that H1H2 and H2H3 implies H1H3, so is transitive. That takes care of partial order axiom 3. Axioms 1 and 2 are equally easy to prove. We also know that HG and {e}H, for all HG, so it is bounded. The only thing that remains to be shown is that this partial order is a lattice. To do that we need to show that and are well-defined. We’ll show that with a couple lemmas, which we’ll prove below.

Lemma (^ is well-defined)

Let G be a group, H1 and H2 be two subgroups, then H1H2 is a subgroup and furthermore H1H2=H1H2.

Proof

Let a and b be in H1H2, then a and b are in both H1 and H2, so by the subgroup test lemma, ab1 in both H1 and H2, so their intersection must be a subgroup. Now, let K be any subgroup where KH1 and KH2. Then since K is a subgroup of both subgroups, it must also be a subset of both subgroups, so we must have KH1H2. This implies that H1H2=H1H2.

QED

I’m starting to think I’ve already proved that the intersection of two subgroups is a subgroup, but at least the proof is very quick.

Lemma (v is well-defined):

Let G be a group, H1 and H2 be two subgroups, then H1H2 is equal to H1K,H2KK.

Proof

G is in this intersection, so it is not an empty intersection. We’ve just shown that the intersection is a subgroup (in fact, in a previous entry, we showed that it’s true even for an infinite amount of subgroups). Clearly, any subgroup to both H1 and H2 will contain this intersection, so it is .

QED

This completes our proof that subgroups form a bounded lattice.

Theorem (when v = *)

Let H, and N be subgroups in G, such that H is also a subgroup of NG(G), the normalizer of N in G. That is, for all hH, we have h1Nh=N, then HN=HN.

Proof

Clearly HN is a subgroup of G which contains both H and N. Therefore, we only need to show that there is no strictly smaller subgroup which contains both. This is straight-forward.

Let K be a subgroup such that HK and NK, then for any hH, and any nN, hK and nK. Now, since K is a subgroup, hnK. Therefore, HNK, thus HN=HN.

QED

Unfortunately, when H isn’t in the normalizer of N, we don’t have this nice relationship.

I’ve mentioned before that what I’ve used as the definition for HN isn’t typical. It’s more common to define HN, (also written simply as HN, as {hn|hH,nN}. This definition is preferable when we don’t necessarily know that H, and N are subgroups of a group G, or when we’re not sure that HNG(N), because it is always equal to a subset of G (but not necessarily a subgroup of G). From now on, I’ll also use that as the definition of HN, and treat the formula HN=α1α(H) more like the result of a theorem, instead.

Theorem (HK = KH implies it is a subgroup)

Let H and K be two subgroups of a group G, then HK=KH implies HK is a subgroup.

Proof

Suppose HK=KH, then let a=h1k1 and b=h2k2 be two elements of HK. Then b1=k21h21, so ab1=h1(k1k21)h21. Since K is a subgroup, k1k21=k3, for some k3K. Therefore the product is equal to (h1k3)h21. Now, since HK=KH, h1k3 is equal to k4h4, for some k4K and h4H. Then the product is equal to k4(h4h21), which itself is equal to k4h5, because h4h21=h5, for some h5H, because H is a subgroup.

Therefore, ab1=k4h5KH, which is equal to HK, by assumption, and so by the subgroup test, HK is a subgroup.

QED

The argument in the proof that = above still works here. Thus in this case as well we have HK=HK.

Next, we’re going to introduce

Definition (modular lattice)

Let L be a lattice such that if C, and DL, such that CD, then for any BL, we have (CB)D=(DB)C, then L is said to be a modular lattice.

To better appreciate that definition, here’s a picture of a lattice that is not modular.

Non-modular lattice

Notice that (CB)D=ED=D, whereas (DB)C=CC=C. Therefore, if CD, then the lattice is not modular. You can see that if this lattice were modular, that D=C, so we would not have this pentagon appear without lines inside it. It would instead be a diamond.

It turns out that modular lattices behave fairly nicely.

Theorem (distribution I)

Let L be a lattice, let X, Y, and Z be elements of L, then

X(YZ)(XY)(XZ)

Equality will always hold if L is a modular lattice.

Proof

Notice that X(XY), and X(XZ). We also have, (YZ)Y(XY), so (YZ)(XY). Similarly, (YZ)Z(XZ), so combining these gives us

X(YZ)(XY)(XZ)

So, now we’re left with a sublattice that looks like this

Lattice Distribution I

Where

D=(XY)(XZ)C=X(YZ)

You can see that if the lattice is modular, then, as we showed above, the dashed pentagon cannot occur, so in that case D=C, and we have equality.

QED

The final theorem for this entry will be the dual to the distributive result above.

Theorem (distribution II)

Let L be a lattice, let X, Y, and Z be elements of the lattice, then

X(YZ)(XY)(XZ)

Equality is guaranteed if L is modular.

Proof

We have (XY)X, and (XY)Y(YZ), so (XY)X(YZ). Similarly, (XZ)X(YZ). Therefore, combining the two inequalities, we get

(XY)(XZ)X(YZ)

If the inequality is strict, we end up with the following sublattice

Lattice Distribution II

Where C=(XY)(XZ), and D=X(YZ). This results in a pentagonal sublattice with no interior lines (because there are no interior relations among the five elements of the lattice). This cannot happen in a modular lattice, so we must have C=D if L is modular.

QED

These results might lure you into thinking that we can always get away with swapping with as long as we swap “” with “”, but that isn’t always the case with lattices. As an example, consider the following lattice

Lattice Flip Counter-example

Notice that if CD, then TS1S2, however, TS1S2. We’ll continue this discussion in a later entry…