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,, usually written , which satisfies the following axioms
- , .
- , and implies that .
- , and implies .
When writing out the partial order, we sometimes write it as an ordered pair , 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 with the relation if and only if and , 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, and aren’t comparable as .
Consider a second example of ordered pairs of rationals where if and only if and . Notice that with this partial order on , that for any pair of elements and , we can find a , such that and . To see this, let and be two ordered pairs of rational numbers. Then if we let , we see that and as we wanted. Similarly, by taking , we have and .
However, the first example we gave didn’t have this property. To see that, consider the example pair we gave above, and . There is no which can be comparable to both and , because in that case , the second component of , would have to equal both and .
This brings us to our next few definitions.
Definition (lattice)
Let be a partial order such that for any two elements, and , there exists , such that , , and , then this partial order is said to be a lattice.
Definition (join)
Let be a lattice. Let and , then the -least element , such that and is said to be their join. It is typically written as .
This is also called , 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 . We’ll define that more precisely later.
Definition (meet)
Let be a lattice. Let and , then the -greatest element , such that and is said to be their meet. It is typically written as .
More precisely, , where and implies . The precise definition for is similar. It is sometimes called .
Notice that and are functions which map every element of to another element of , whenever is a lattice. Now we prove that it’s associative.
Definition ( >= )
Let be a partial order. Then we define to be the relation such that , if and only if for all , .
Hopefully that last definition didn’t confuse or surprise anyone.
Theorem ( v is associative):
Let , and be elements of . Let’s be a lattice. Then, .
Proof
Let , and . Also let and . Then we have
Then, by definition, we have , , and . By the transitivity of , we have . Therefore, by the definition of , we have . We also have , which means that applying transitivity again, . This means, that, by the definition of , . A similar argument will show that , and thus by partial order axiom 2.
QED
Theorem ( ^ is associative)
Let , and be elements of . Let’s be a lattice. Then, .
Proof
Very similar to the proof for .
Definition (bounded lattice)
Let be a lattice, such that there are two elements of , which we’ll call and , such that for all , and . Then is said to be a bounded lattice.
Let be a group and let , then , where is the usual subgroup relation, is a bounded lattice.
Proof
By the definition of subgroup, we know that and implies , so is transitive. That takes care of partial order axiom 3. Axioms 1 and 2 are equally easy to prove. We also know that and , for all , 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 be a group, and be two subgroups, then is a subgroup and furthermore .
Proof
Let and be in , then and are in both and , so by the subgroup test lemma, in both and , so their intersection must be a subgroup. Now, let be any subgroup where and . Then since is a subgroup of both subgroups, it must also be a subset of both subgroups, so we must have . This implies that .
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 be a group, and be two subgroups, then is equal to .
Proof
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 and will contain this intersection, so it is .
QED
This completes our proof that subgroups form a bounded lattice.
Theorem (when v = *)
Let , and be subgroups in , such that is also a subgroup of , the normalizer of in . That is, for all , we have , then .
Proof
Clearly is a subgroup of which contains both and . Therefore, we only need to show that there is no strictly smaller subgroup which contains both. This is straight-forward.
Let be a subgroup such that and , then for any , and any , and . Now, since is a subgroup, . Therefore, , thus .
QED
Unfortunately, when isn’t in the normalizer of , we don’t have this nice relationship.
I’ve mentioned before that what I’ve used as the definition for isn’t typical. It’s more common to define , (also written simply as , as . This definition is preferable when we don’t necessarily know that , and are subgroups of a group , or when we’re not sure that , because it is always equal to a subset of (but not necessarily a subgroup of ). From now on, I’ll also use that as the definition of , and treat the formula more like the result of a theorem, instead.
Theorem (HK = KH implies it is a subgroup)
Let and be two subgroups of a group , then implies is a subgroup.
Proof
Suppose , then let and be two elements of . Then , so . Since is a subgroup, , for some . Therefore the product is equal to . Now, since , is equal to , for some and . Then the product is equal to , which itself is equal to , because , for some , because is a subgroup.
Therefore, , which is equal to , by assumption, and so by the subgroup test, is a subgroup.
QED
The argument in the proof that above still works here. Thus in this case as well we have .
Next, we’re going to introduce
Definition (modular lattice)
Let be a lattice such that if , and , such that , then for any , we have , then is said to be a modular lattice.
To better appreciate that definition, here’s a picture of a lattice that is not modular.

Notice that , whereas . Therefore, if , then the lattice is not modular. You can see that if this lattice were modular, that , 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 be a lattice, let , , and be elements of , then
Equality will always hold if is a modular lattice.
Proof
Notice that , and . We also have, , so . Similarly, , so combining these gives us
So, now we’re left with a sublattice that looks like this

Where
You can see that if the lattice is modular, then, as we showed above, the dashed pentagon cannot occur, so in that case , and we have equality.
QED
The final theorem for this entry will be the dual to the distributive result above.
Theorem (distribution II)
Let be a lattice, let , , and be elements of the lattice, then
Equality is guaranteed if is modular.
Proof
We have , and , so . Similarly, . Therefore, combining the two inequalities, we get
If the inequality is strict, we end up with the following sublattice

Where , and . 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 if 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

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