Show that inner product is zero.

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Discussion Overview

The discussion revolves around proving that the inner product of eigenkets corresponding to different eigenvalues of a Hermitian operator is zero. It explores the implications of the commutation of operators and the properties of Hermitian and self-adjoint operators within the context of quantum mechanics.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents the problem of showing that \(\langle u_i | B | u_j \rangle = 0\) for \(a_i \neq a_j\) given that \(A\) is a Hermitian operator and \(B\) commutes with \(A\).
  • Another participant questions whether \(A\) is Hermitian or self-adjoint, suggesting that if \(A\) is self-adjoint, the result follows directly from the properties of eigenkets and eigenbras.
  • A different participant claims to have derived the result using the Hermiticity of \(A\) and concludes that \(\langle u_i |B| u_j \rangle = 0\) under the condition \(a_i \neq a_j\).
  • One participant raises a technical point about the distinction between Hermitian and self-adjoint operators, noting that the property of eigenbras may not hold if \(A\) is only Hermitian.
  • Another participant expresses agreement with the previous points and emphasizes the importance of understanding the implications of commuting operators and their common eigenvectors.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of Hermitian versus self-adjoint operators. While some participants agree on the mathematical steps leading to the conclusion, the discussion remains unresolved regarding the implications of these definitions.

Contextual Notes

The discussion highlights the potential confusion surrounding the terms Hermitian and self-adjoint, particularly in the context of quantum mechanics versus pure mathematics. There is also an acknowledgment of the complexity involved in the Dirac bra-ket formalism.

perishingtardi
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Let A be a Hermitian operator with n eigenkets: A|u_i\rangle = a_i |u_i\rangle for i=1,2,...,n.

Suppose B is an operator that commutes with A. How could I show that
\langle u_i | B | u_j \rangle = 0 \qquad (a_i \neq a_j)?

I have tried the following but not sure how to proceed:
AB - BA=0\\ \implies \langle u_i | AB | u_j \rangle - \langle u_i | BA | u_j \rangle = 0
 
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Is ##A## Hermitian or is it self-adjoint? If it is the latter then the result is immediate from what you wrote down because for any self-adjoint operator ##A##, if ##|u_i \rangle## is an eigenket of ##A## with eigenvalue ##a_i## then ##\langle u_i|## is an eigenbra of ##A## with the same eigenvalue i.e. ##\langle u_i|A = a_i\langle u_i |## so you would be left with ##(a_i -a_j) \left \langle u_i|B|u_j \right \rangle = 0##.
 
Actually I think I got it:

a_i \langle u_i |B|u_j \rangle - \langle u_i |B| u_j \rangle a_j = 0 using the Hermiticity of A for the first term, and then since a_i \neq a_j we get
\langle u_i |B| u_j \rangle = 0
 
This is a technical point and I don't know if it matters for your class however it should be noted that while ##\langle u_i |A = a_i \langle u_i |## is certainly true if ##A## is self-adjoint, it won't necessarily be true if ##A## is only Hermitian.
 
WannabeNewton said:
Is ##A## Hermitian or is it self-adjoint? If it is the latter then the result is immediate from what you wrote down because for any self-adjoint operator ##A##, if ##|u_i \rangle## is an eigenket of ##A## with eigenvalue ##a_i## then ##\langle u_i|## is an eigenbra of ##A## with the same eigenvalue i.e. ##\langle u_i|A = a_i\langle u_i |## so you would be left with ##(a_i -a_j) \left \langle u_i|B|u_j \right \rangle = 0##.

Thanks for that - I think we both posted at the same time! My question is related to quantum mechanics. I think physicists use the words Hermitian and self-adjoint interchangeably. I know that pure mathematicians will distinguish them but it's not important for my area. Thanks!
 
Alrighty then! Glad you got it worked out :)
 
Just by using the Dirac bra-ket formalism (one of the most vicious inventions in the history of science) means that you're hiding a lot of mathematical beauty under the carpet. Let's proceed then and leave finesse aside and say that if A and B commute, then they have a common set of eigenvectors. Thus the ui's of A are the ui's of B, so that you need to prove that 2 eigenvectors pertaining to 2 different eigenvalues are orthogonal one on each other.
 

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