Operator with 3 degenerate orthonormal eigenstates

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SUMMARY

The discussion centers on the operator ##\hat{A}## with three degenerate orthonormal eigenstates, where the diagonal elements of ##\hat{A}## are confirmed to equal the eigenvalue ##a##. The matrix representation of ##\hat{A}## is given as ##\hat{A} = \begin{bmatrix} a & A_{12} & A_{13} \\ A_{21}& a & A_{23}\\A_{31} & A_{32} & a \end{bmatrix}##. Participants seek clarification on how to derive the commuting relation from this matrix and the implications of normalized linear combinations of the eigenstates being eigenstates of ##\hat{A}## with eigenvalue ##a##. The distinction between the equations ##\hat{A} |n\rangle = a|n\rangle## and ##\langle n \lvert \hat{A} \rvert n \rangle = a## is also highlighted.

PREREQUISITES
  • Understanding of linear algebra concepts, particularly eigenvalues and eigenvectors.
  • Familiarity with matrix representation of operators in quantum mechanics.
  • Knowledge of degenerate states and their implications in quantum systems.
  • Basic grasp of the commutation relations in quantum mechanics.
NEXT STEPS
  • Study the properties of degenerate eigenstates in quantum mechanics.
  • Learn about the implications of commuting operators and their significance in quantum theory.
  • Explore the concept of normalized linear combinations of eigenstates and their eigenvalue relationships.
  • Investigate the mathematical derivation of commuting relations from matrix representations of operators.
USEFUL FOR

Quantum physicists, students of quantum mechanics, and researchers exploring the properties of operators with degenerate eigenstates will benefit from this discussion.

Celso
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Homework Statement
I've been given an operator ##\hat{A}## that has 3 orthonormal vectors as degenerate eigenstates corresponding to the same eigenvalue ##a##.

I know how the hamiltonian acts on these vectors and I want to use this information to check whether ##\hat{H}## and ##\hat{A}## commute or not.
Relevant Equations
## \hat{A} |1> a|1>, \hat{A} |2> a|2>, \hat{A} |3> a|3>##
##\hat{H} = \begin{bmatrix} \sigma & 0 & \sigma \\ 0 & \sigma & \delta \\ \sigma & \delta & \sigma \end{bmatrix} ##
With this information I concluded that the diagonal elements of ##\hat{A}## are equal to the eigenvalue ##a##, so ##\hat{A} = \begin{bmatrix} a & A_{12} & A_{13} \\ A_{21}& a & A_{23}\\A_{31} & A_{32} & a \end{bmatrix}## but I can't see how to go from this to the commuting relation, since I don't know the other terms.
 
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Can you show that any normalized linear combination of the three orthonormal vectors is also an eigenstate of ##\hat A## with eigenvalue ##a##? If you can, what does this have to do with the question being asked here?
 
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Celso said:
Relevant Equations:: ## \hat{A} |1> a|1>, \hat{A} |2> a|2>, \hat{A} |3> a|3>##

With this information I concluded that the diagonal elements of ##\hat{A}## are equal to the eigenvalue ##a##, so ##\hat{A} = \begin{bmatrix} a & A_{12} & A_{13} \\ A_{21}& a & A_{23}\\A_{31} & A_{32} & a \end{bmatrix}## but I can't see how to go from this to the commuting relation, since I don't know the other terms.
Note that your relevant equations say ##\hat{A} |n\rangle = a|n\rangle##, not ##\langle n \lvert \hat{A} \rvert n \rangle = a##.
 

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