Hermitian Operator Proof - Question

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SUMMARY

The discussion focuses on the necessity of a specific proof related to Hermitian operators in quantum mechanics, particularly regarding the computation of the complex conjugate of the expectation value of a physical variable. Participants emphasize that proving the eigenvalues of Hermitian operators are real is crucial, as this leads to the orthogonality of eigenfunctions corresponding to different eigenvalues. The proof referenced is essential for understanding the properties of observables in quantum mechanics.

PREREQUISITES
  • Understanding of Hermitian operators in quantum mechanics
  • Familiarity with expectation values in quantum mechanics
  • Knowledge of eigenvalues and eigenfunctions
  • Basic principles of quantum mechanics and linear algebra
NEXT STEPS
  • Study the proof of the eigenvalues of Hermitian operators
  • Learn about the orthogonality of eigenfunctions in quantum mechanics
  • Explore the implications of complex conjugates in quantum expectation values
  • Investigate non-Hermitian operators and their properties
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Students and researchers in quantum mechanics, physicists focusing on operator theory, and anyone seeking to deepen their understanding of Hermitian operators and their significance in quantum observables.

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 < H\psi \mid \psi > ?
 
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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 < H\psi \mid \psi > ?

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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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 < H\psi \mid \psi > ?

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

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