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.