Lecture 4 - Duality (intro)

Recall that:

T~

Suppose TL(V,W). Define T~:V/(null(T))W by:
T~(v+null(T))=Tv

What we're doing here is if you collect all things that were in null(T), then that makes T~ is injective. Thus, it's an isomorphism between V/null(T) and range(T).

Really the injectivity comes from the fact that the only thing that get's mapped to 0W is anything in 0+null(T)=null(T). Like how a function cannot have multiple possible outputs, here we can only have multiple possible different inputs to the same output in W.

Consider the Following

Suppose now that I have U which is a subspace of V. Let's suppose I have TL(V). The question is:

Question

When is the map S:V/UV/U defined by:

S(v+U)=T(v)+U

well defined?

Consider when it's a problem. It's problem if we get two different outputs for the same input. Given v1+U=v2+U, we need there images under S to be equal. Checking this, notice that we must have v1v2U:

S(v1+U)=S(v2+U)T(v1)+U=T(v2)+UT(v1)T(v2)U

So then T(v1v2)U. This means we need U to be a T-invariant subspace. This is equivalent to null(T)U (this is actually a stronger condition for the T-invariance).

It's also an if and only if, interestingly enough.

Recall from last quarter that there was the following theorem:

Over C, every operator has an upper-triangular matrix

Suppose V is a finite-dimensional complex vector space and TL(V). Then T has an upper-triangular matrix with respect to some basis of V.

We had a proof in the book that was a bit weird, but let's do a new one.

We use the fact that every operator T on a finite-dimensional complex vector space has at least one eigenvalue. The idea was to take T:VV, which has λ1 as an eigenvalue, has an associated eigenvector v1. We start making the list {v1}. We consider Tv1=λ1v1 so then T is invariant over span(v1).

As such, S is well-defined, so then create T1:V/span(v1)V/span(v1), where T1(v+span(v1))=Tv+span(v1). Notice the dimension of V/span(v1) is n1 dimensional space.

But now this map T1 itself has an eigenvalue since it's a finite-dimensional complex vector space and T1L(V/span(v1)). It has an eigenvalue λ2 with eigenvalue v2+span(v1). Note that:

T1(v1+span(v1))=λ2v2+span(v1)

by definition. As such, v2 is not in the span of v2 because if it were then the λ2v2=0 but v2 cannot zero since it's an eigenvector. As such, we have the list {v1,v2} which is a LI list.

Now look at T2:V/span(v1,v2)V/span(v1,v2) defined in the same way. We can repeat this process n times.

We eventually get the list {v1,...,vn}. It's a basis as the list is LI and is the right length. Note that also T(vi)span(v1,...,vi) to show the UT part.

Notice that v2,...,vn are not eigenvectors of T. Rather, they are eigenvectors of T2,...,Tn respectively.

Duality

We defined

Definition

A linear functional on V is an element of L(V,F).

for instance, the trace of a matrix is a functional. Another one is ϕ:P(R)R defined by:

ϕ(p)=p(0)+p(1)+p(2)

Notice that dim(L(V,F))=dim(V). Since these are the same, then these spaces are isomorphic

Definition

The vector space L(V,F) is called the dual space of V. It is denoted:

V

then V and V are isomorphic, assuming V is finite-dimensional.