Determining Hermitian Operators: Cases 1 and 2

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Homework Help Overview

The discussion revolves around determining whether specific operators are Hermitian within the context of quantum mechanics. The operators in question are defined by their actions on wave functions, with one operator involving a translation and the other involving complex conjugation.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the definitions and properties of Hermitian operators, considering cases where the operator acts on functions. There is a mention of using inner products to verify the Hermitian property, as well as checking symmetry conditions for the operators.

Discussion Status

The discussion includes attempts to clarify the conditions under which the operators can be considered Hermitian. Some participants provide guidance on using inner products and symmetry checks, while others reiterate the need for a clear understanding of the definitions involved.

Contextual Notes

Participants reference the Hilbert space of square-integrable functions and the scalar product used in this context, indicating a focus on mathematical rigor in the analysis of the operators.

James R
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My memory is fading. Can somebody please remind me how I would go about determining in each of the following cases whether the operator A is Hermitian or not?

Case 1.

[tex]A\psi(x) = \psi(x+a)[/tex]

Case 2.

[tex]A\psi(x) = \psi^*(x)[/tex]

where the star indicates complex conjugation.
 
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James R said:
My memory is fading. Can somebody please remind me how I would go about determining in each of the following cases whether the operator A is Hermitian or not?

Case 1.

[tex]A\psi(x) = \psi(x+a)[/tex]

Case 2.

[tex]A\psi(x) = \psi^*(x)[/tex]

where the star indicates complex conjugation.

take two vectors, f and g. In your case, these are functions of x.
Now calculate ff = A f and gg = A g.
If A is hermitean, then <gg,f> = <g,ff> for all f and g.
 
Assume for simplicity that [itex]\hat{A}[/itex] is an linear operator continuous on the Hilbert space [itex]L^{2}\left(\mathbb{R}\right)[/itex] in which the scalar product between 2 arbitrary vectors is

[tex]\langle \psi,\phi \rangle =\int_{-\infty}^{+\infty} dx \ \psi^{*}(x) \phi (x)[/tex].

If an operator described above is symmetric, then

[tex]\langle \psi, \hat{A}\phi\rangle =\langle \hat{A}\psi, \phi\rangle , \forall \psi,\phi \in \mathcal{H}[/tex]

So check both operators now.

Daniel.
 
Thanks.....
 

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