Hermitian Operator Proof - Question

In summary: This is done for the very specific reason that it will make the expansion of a function in terms of the eigenfunctions unique and consistent.In summary, the conversation is about the need for a specific proof to compute the complex conjugate of the expectation value of a physical variable. The need for this proof arises from the requirement to prove that the eigenfunctions of a Hermitian operator are orthogonal, which is necessary for a unique and consistent expansion of a function in terms of the eigenfunctions.
  • #1
Jd_duarte
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Hi,

I am questioning about this specific proof -https://quantummechanics.ucsd.edu/ph130a/130_notes/node134.html.
Why to do this proof is needed to compute the complex conjugate of the expectation value of a physical variable? Why can't we just start with [itex] < H\psi \mid \psi > [/itex] ?
 
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  • #2
Jd_duarte said:
Hi,

I am questioning about this specific proof -https://quantummechanics.ucsd.edu/ph130a/130_notes/node134.html.
Why to do this proof is needed to compute the complex conjugate of the expectation value of a physical variable? Why can't we just start with [itex] < H\psi \mid \psi > [/itex] ?

If that's a proof of anything, it escapes me.

Normally, one proves that the eigenvalues of a Hermitian operator are real and then attention is restricted to Hermitian operators for observables; even though there may be non-Hermitian operators with real eigenvalues.
 
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  • #3
Jd_duarte said:
Hi,

I am questioning about this specific proof -https://quantummechanics.ucsd.edu/ph130a/130_notes/node134.html.
Why to do this proof is needed to compute the complex conjugate of the expectation value of a physical variable? Why can't we just start with [itex] < H\psi \mid \psi > [/itex] ?

Because you will need that result to prove that the eigenfunctions of an hermitian operator corresponding to different eigenvalues are orthogonal.
 

1. What is a Hermitian operator?

A Hermitian operator is a mathematical object that operates on a vector in a complex vector space. It is defined as an operator that is equal to its own conjugate transpose.

2. How is a Hermitian operator different from a normal operator?

A normal operator is an operator that commutes with its adjoint, while a Hermitian operator is an operator that is equal to its own adjoint. This means that a Hermitian operator is a special case of a normal operator.

3. What is the significance of Hermitian operators in quantum mechanics?

In quantum mechanics, Hermitian operators represent physical observables, such as position, momentum, and energy. The eigenvalues of Hermitian operators correspond to the possible outcomes of measurements of these observables.

4. How do you prove that an operator is Hermitian?

To prove that an operator is Hermitian, you need to show that it is equal to its own adjoint. This can be done by taking the adjoint of the operator and showing that it is equal to the original operator.

5. Can a non-square matrix be a Hermitian operator?

No, a non-square matrix cannot be a Hermitian operator. Hermitian operators are defined for square matrices in complex vector spaces. Non-square matrices cannot have an adjoint, which is necessary for an operator to be Hermitian.

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