Discussion Overview
The discussion revolves around the relationship between a Hermitian operator A and the Hamiltonian H in quantum mechanics, specifically whether they share a set of eigenfunctions if they commute. Participants explore the implications of this relationship for time evolution and the conditions under which eigenvectors are shared.
Discussion Character
- Technical explanation
- Debate/contested
- Mathematical reasoning
Main Points Raised
- One participant states that if the time evolution of a ket is expressed in terms of the Hamiltonian, it raises the question of whether operator A and the Hamiltonian share eigenfunctions, implying they commute.
- Another participant proposes that if the eigenvalues of A, denoted as ##E_a## and ##E_b##, are not equal, then A and H share the same eigenvectors. However, if the eigenvalues are equal, linear combinations of the eigenvectors of A may still be eigenvectors of H, complicating the relationship.
- A further participant questions the reasoning behind the assertion that A and H share eigenvectors when the eigenvalues are distinct.
- Another participant provides a mathematical argument stating that if the commutator of A and H is zero and the spectrum of H is non-degenerate, then the matrix representation of A is diagonal in the basis of eigenstates of H, indicating that they share eigenvectors.
Areas of Agreement / Disagreement
Participants express differing views on the conditions under which A and H share eigenfunctions, particularly regarding the implications of equal versus unequal eigenvalues. The discussion remains unresolved as participants explore these nuances.
Contextual Notes
Participants do not reach a consensus on the implications of the eigenvalue conditions or the general relationship between the operators, leaving several assumptions and mathematical steps unresolved.