Discusses basic properties and classifications of operators.
We start with a simple but useful property.
Lemma 1 If
and
for all
, then
.
Let
, then for any
, we have that
. Therefore, we obtain
Since
, we have that
;
therefore,
.
If we set
, then
. So in this case,
.
If we set
, then
. So in this case,
.
Thus,
for all
, which means
for all
.
So we can come to the conclusion that
.
Solutions to operator equations
Assume
and
are two normed linear spaces and
is a bounded linear operator. Now pick
. Then we pose the question: does a solution
to the equation
exist?
There are three possibilities:
- A unique solution exists;
- multiple solutions exist; or
- no solution exists.
We consider these cases separately below.
-
Unique solution : Assume
and
are two solutions to the equation. In this case we have
. So
. Therefore,
. If the solution
is unique then we must have
and
. Therefore,
. Since the operator has a trivial null space, then
exists. Thus, the solution to the equation is given by
;
-
Multiple solutions : In this case, we may prefer to pick a particular solution. Often, our goal is to find the solution with smallest norm (for example, to reduce power in a communication problem). Additionally, there is a closed-form expression for the minimum-norm solution to the equation
.
Theorem 1 Let
,
be Hilbert spaces,
, and
. Then
is the solution to
if and only if
, where
is the solution of
.
Let
be a solution to
. Then all other solutions can be written as
, where
.
We therefore search for the solution that achieves the minimum value of
over
, i.e., the closest point to
in
.
Assume
is such a point; then,
. Now, recall that
, so
.
Thus
for some
, and
.
Note that if
is invertible, then
.
-
No solution : In this case, we may aim to find a solution that minimizes the mismatch between the two sides of the equation, i.e.,
. This is the well-known projection problem of
into
.
Theorem 2 Let
,
be Hilbert spaces,
, and
. The vector
minimizes
if and only if
.
Denote
so that
. We need to find the minimum value of
over
. Assume
is the closest point to
in
,
then
, which means
. Recall that
, which implies that
.
So
. Thus
. Now, denoting
, we have that
.
Note that if
is invertible, then we have
.
Unitary operator
Definition 1 An operator
is said to be
unitary if
.
This implies that
. Unitary operators have norm-preservation properties.
Theorem 3
is unitary if and only if
and
for all
.
Let
be unitary, then for any
,
Since
and
, then
. So if
is unitary, then
and
for all
.
From
[link] we can find that
Since this is true for all
we have that
for all
, which means that
for all
. Therfore, we must have
. Additionally, since the operator is unitary, we find that for any
we have that
. So
if and only if
, implying that
is one-to-one.
Since
, then
is onto as well. Thus,
is invertible, which means
. So
, and therefore
. The result is that
is unitary. We have shown that if
and
for all
, then
is unitary.
Corollary 4 If
is finite-dimensional, then
is unitary if and only if
for all
.