Lecture 15 - Finishing 7C, More Applications of Linear!
Recall how we defined a positive operator:
positive operator
An operator is called positive if is self-adjoint and:
for all .
Recall we needed and thus required that to be self-adjoint.
Like with complex numbers, we want to show how 's of operators stay within this positive realm.
Properties of positive operators
is self-adjoint, the following are equivalent:
is positive
is self-adjoint and all eigenvalues of are non-negative.
has a positive square root (we will show that this is unique later).
has a self-adjoint square root.
There exists an operator such that .
Proof
We prove (a) (b) ... (e) (a). Notice that:
(d) implies (e) is pretty obvious.
(c) implies (d) comes from the fact that 's square root must be self-adjoint as is already self-adjoint.
(a) (b): Suppose is positive. Let for some non-zero vector . Then:
via the definition. Since so then and we are done.
(b) (c): There is an orthonormal eigenbasis for (via the Spectral Theorem) w/ e-vals . Then:
where is given by . This is allowed since each so taking the square root is fine here. is 's positive square root, where the positivity comes from so then:
(e) (a): Suppose there is such that :
so is positive.
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Uniqueness of a positive square root of an operator
The positive square root of a positive operator is unique.
Proof
Use from the previous proof. We'll show that is unique. Suppose for some positive operators . Start with (a positive operator, thus self-adjoint and ...), given an orthonormal eigenbasis for , say .
We'll show that any (this is the operator defined in (b) (c) in the previous proof). Since is positive, then it has its own orthonormal eigenbasis with eigenvalues (notice that these are still arbitrary and positive, per our requirement). Write:
Thus or for each . Note that , so throw out the terms without the :