Lecture 5 - Continuing Duality

Recall the idea of a linear functional:

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.

Note that when V is finite dimensional:

dim(V)=dim(V)

so then V and V are isomorphic. However, if it's infinite-dimensional, then it's possible where no isomorphism exists.

The idea of finding these isomorpisms was to find the basis vectors and map from one basis to the other. As such, we'll define the dual basis:

dual basis

Given a basis β={v1,...,vn} of V, the dual basis of β is ϕ1,...,ϕnV where:

ϕj(vk)={1k=j0kj=χ(k=j)

for all j. Here χ returns 1 if the statement is true, and 0 when false.

Here the ϕj is a valid linear functional, defining it by its action on a basis. We need to prove that it's actually a basis for V below.

Proof
We already have n ϕ's, which is the dimension of V. As such, we'll just show LI.

Consider when:

a1ϕ1++anϕn=0

where 0 is the linear functional in this case. Consider some arbitrary basis vector viV. Then:

(a1ϕ1++anϕn)(vi)=0=a1ϕ1vi++anϕnvi

But then this implies that all ai=0 since the only basis vector vi that allows something non-zero is the i-th one. As such, then ai=0 for all i, so then the set of vectors is LI.

Basis gives ϕ's

Note that this whole process depended on the basis v1,...,vn that we started with. If you change the basis, you're ϕ's will change as a result.

Dual Maps of T

As the picture shows, note that we can build a linear map from V to F by doing T then ϕ (which combined gives ϕT. As such, we construct the dual map:

dual map

If TL(V,W) then the dual map of T is TL(W,V) defined by:

T(ϕ)=ϕT

for all ϕW.

As a fact, this map T is linear.

As an example, define TFn,n by:

T([11a1an11])=[11ana111]

Here it maps from Fn,n to itself. Let tr be the trace functional on Fn,n. What is T(tr)? We can figure this out via:

T(tr)=trT

So what does this trT do to a matrix like we have above. It's:

(trT)([a11a1nan1ann])=tr([a1na11annan1])=i=1nai,n+1i

These are pretty funky, so let's do another example. Let V,W be vector spaces. Let e1,e2 be a basis for V and f1,f2,f3 be a basis for W. Suppose TL(V,W) where M(T,βV,βW) is a 3x2 matrix:

[abcdef]

What about the dual map T? We know that we have ϕ1,ϕ2 as the dual basis for βV and ψ1,ψ2,ψ3 is the dual basis for W. Here TL(W,V). Hence, the matrix must be instead 2x3 (hint: look at the dimensions for W,V).

The columns of the matrix represent to the image T(ei) in this case for what parts of the basis compose the basis. So:

T(e1)=af1+cf2+ef3,T(e2)=bf1+df2+ff3

What is M(T,βW,βV) (the ψ's go first here)? Just look at the image of each basis vector:

T(ψ1)=ψ1T

So for example:

T(ψ1)(e1)=(ψ1)(Te1)=(ψ1)(af1+cf2+ef3)=aT(ψ1)(e2)=(ψ1)(Te2)=(ψ1)(bf1+df2+ff3)=b

Because the ψ1 just gets the constant amount of f1 as defined. So the first column of the matrix is:

[acebdf]

WHICH IS THE TRANSPOSE OMG!!!.