Lecture 11 - Starting Infinite Dimensional Spaces!

Recall what we covered in Lecture 10 - Finishing LI&LD, Bases#Bases. We made a system to show that the length of a LI list is the length of a spanning list, by doing the "booting" process, where you boot out each v one at a time by adding a u each step:

u1,v1,...,vmu2,u1,v1,...,vm1un,...,u1,vj,...

Where since we eventually run out of v's then the number of u's is less than the number of v's.

Infinite Dimensional Spaces

Let's get back into dimension. Recall that two unique bases in a vector space V, they have the same list length, which we the name of dimension. However, we might've jumped the gun, since we may not be finite dimensional. But first, what is that?

Finite Dimensional

A vector space V is called finite-dimensional if there is a spanning list for V of finite length.

Note that the spanning list doesn't need to have the dimensions' number of vectors. We may have extras! But we can always trim it back down to a basis via Lecture 10 - Finishing LI&LD, Bases#Reduction.

Infinite Dimensional

We say V is infinite-dimensional if it is not finite dimensional, so there is no finite spanning list for V.

For instance, P(R), the space of all polynomials with real coefficients, is infinite-dimensional. But to prove it you prove that, for contradiction, if you had a finite spanning list for the space, then if you can create a vector not in that span that's still in V, then you did it! For our space in question, if we had a spanning list we'd have some maximum degree xn, which doesn't include xn+1, which completes the proof.

Example

The dimension of Pn(R) is n+1 (since we include our 0-degree term). We can use {1,x,x2,...,xn} is a basis of that size for Pn(R).

Let's do a cool proof!

Theorem

If V is a F.D.V.S. and U is a subspace of V, then U is F.D. and dim(U)dim(V).

Proof
We can't just use V's spanning list to make a spanning list for U, since the vectors that are in that spanning list may not necessarily be in U. So we need to construct a new spanning list for it.

If U={0}, then the empty list {} is the spanning list and we are done, as it is F.D.
If U{0} then there is some vector u1U. Consider span(u1). This list is LI already. If the span is U itself then we are done. If it doesn't, then choose another vector u2U such that u2span(u1). If we consider span(u1,u2), then this is LI, since we are adding a vector that isn't in the span of the previous list.

We repeat this process.

We always create a longer and longer LI list. But they can't be longer than the the spanning list for V, which is finite dimensional, say some dimension n. Then we must have the new spanning list at the end span(u1,...,ui) must be smaller than n, so then dim(U)dim(V). Furthermore, as a result we must terminate, so then U is F.D.

Really, dim(U)dim(V) comes from the Lecture 10 - Finishing LI&LD, Bases#Finishing 2.A, ie the Linear Independence Lemma, and V being finite dimensional.

Note that you have to construct this list, instead of using the list that spans V. Even though it is LI, the subset of vectors that are in U may suddenly not be LI, which is the problem. So this process is needed.

There are also countably-infinite dimensional vector spaces like Pn(R), where a bijection is made from each basis vector and N. Furthermore, there's uncountably-infinite dimensional vector spaces, like the space of all functions RR. However, the pretty results we get are based on being finite dimensional, so we'll focus on that until we get to the end of the quarter.

Theorem

For every subspace U of a finite-dimensional vector space V, there is a subspace W such that:

UW=V

Proof
We need to prove that UW={0}.

Since U is a subspace of finite-dimensional V, then U is finite dimensional, so let u1,...,uk be said basis for U. Now, extend this basis to a basis for V via:

u1,...,uk,v1,...,vnk

Where the nk is from V being n dimensional. This whole list has k vectors. Consider just:

v1,...,vnk$$Wecanjustchoose$W=span(v1,...,vnk)$.Toshowthedirectsumpart,wefirstshowjustthesumpart,whichiseasysincethelist:

u_1, ..., u_k, v_1, ..., v_

Spans$U+W$bydefinition.Forthedirectsumpart,wejustshow$UW={0}$.Sincevectorsinabasisareuniquelywrittenbyeachofourbasis$u1,...,uk$and$v1,...,vnk$,thenavectorin$V$mustbeuniquelywrittensolelybyvectorsinoneortheother.