Reitz Representation Theorem
Every bounded element of can be represented in this way. (This map is an isomorphism between the space and the dual space)
We say is ``dual’’ to and often write , the adjoint of .
What is the relation between them?
Constructive Proof. Choose an orthonormal basis for and let be corresponding dual basis . Note . (Then our map associates the basis dual to an orthonomal basis to the dual basis).
Every can be written as a linear combination of the dual basis and that . Write . Thus, . Thus .
Note
From now on, we will (almost) always use this equivalence to write the inner product in the form you’re accustomed to from QM.
Representations
- - Column vector
- - Row vector
- (Transpose notation is the tilde over the expression in PH562)
Adjoint of an Operator
Definition
The adjoint of an operator is the operator which satisfies .
Implications
If we define by .
Then . Thus, .
So, . Proof. .
- Matrix Represenatation of Operators
Recall we defined .
Then,
Riesz Lemma
is isomorphic to ( is an inner product space).
Author: Christian Cunningham
Created: 2024-05-30 Thu 21:15
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