Diagonal Matrix & Perturbation Theory in Quantum Mechanics

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Discussion Overview

The discussion revolves around the concept of diagonal matrices in the context of Quantum Mechanics, particularly focusing on their relevance to Perturbation Theory and degeneracy. Participants seek clarification on these concepts and their implications in quantum systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants explain that a diagonal matrix has non-zero entries only on its main diagonal, providing a basic definition relevant to finite dimensional vector spaces.
  • Others elaborate that in Quantum Mechanics, a diagonal operator indicates that the basis vectors are eigenvectors, which yield specific values for the associated properties.
  • A participant mentions that an operator is considered diagonal in a particular basis if the matrix elements are non-zero only when the indices are equal, suggesting a connection to eigenstates.
  • One participant expresses difficulty in understanding Perturbation Theory, especially in its degenerate case, and seeks further clarification on the role of matrices in this context.

Areas of Agreement / Disagreement

Participants generally agree on the basic definition of diagonal matrices and their significance in Quantum Mechanics. However, there is no consensus on the specifics of Perturbation Theory and its application to degenerate cases, as some participants find the topic vague and seek further explanation.

Contextual Notes

The discussion highlights the complexity of applying the concept of diagonal matrices to infinite dimensional spaces typical in Quantum Mechanics. There are also unresolved aspects regarding the specifics of Perturbation Theory and its implications for degenerate states.

Who May Find This Useful

Readers interested in Quantum Mechanics, particularly those exploring linear algebra applications in quantum theory, and individuals seeking clarification on Perturbation Theory and degeneracy may find this discussion relevant.

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What does it mean for a matrix to be diagonal, especially in Quantum Mechanics, where we get to Perturbation theory (Degeneracy).
I don't get it. Please if you can explain in 'simple' language.
 
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For finite dimensional vector spaces, a "diagonal matrix" is something like
\begin{bmatrix}a & 0 & 0 \\ 0 & b & 0 \\ 0 & 0 & c\end{bmatrix}
having non-zero entries only on the main diagona. But I suspect you already knew that!

More generally, a square matrix represents a linear operator on some vector space. If that that vector space has finite dimension, n, then we can represent the operator as a n by n matrix. If the vector space is infinite dimensional is, as is typically the case in Quantum theory, we can't really write it as a "matrix" but the same ideas work.

The matrix is "diagonal" in a particular basis, \{v_1, v_2, ..., v_n\} then the basis vectors are eigenvectors: Av_i= a_iv_i where a_i is the number, on the diagonal, at the ith row and column. To say that an operator in Quantum Mechanics is "diagonal" also means that the basis vectors are all eigenvectors (eigenstates). Physically, "eigenstates" are those that give specific values to whatever the property is associated to the state while vectors that are not eigenstates can be written as linear combinations of the eigenstates and then give "mixtures" of those values.
 
Your question is pretty vague, so it's going to be hard to offer any concrete help. Here is what a diagonal matrix is in general: http://en.wikipedia.org/wiki/Diagonal_matrix

In QM, we say an operator ##\hat{A}## is diagonal in some basis of states ##| \psi_i\rangle## (where i is some index labeling the states) if ##\langle \psi_i | \hat{A} | \psi_j \rangle## is only nonzero when ##i = j##.
 
Thank you, but I suppose it was really vague. I am having a hard time understanding Perturbation theory in its degenerate case.
Anything on that matter could help especially the usage of Matrix in that section..
 

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