Symmetric, irreducible, tridiagonal matrix: Eigenvalues

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SUMMARY

The discussion focuses on the properties of symmetric, irreducible, tridiagonal matrices and their eigenvalues. It establishes that such matrices cannot possess multiple eigenvalues, utilizing the Jordan canonical form of the matrix A - λI as a key analytical tool. Additionally, it addresses upper Hessenberg matrices, asserting that if they have a multiple eigenvalue, only one eigenvector can be associated with it. These conclusions are drawn from the definitions and properties of the matrix types involved.

PREREQUISITES
  • Understanding of symmetric matrices and their properties
  • Knowledge of irreducible matrices and their implications
  • Familiarity with tridiagonal and upper Hessenberg matrices
  • Concept of Jordan canonical form and its application in linear algebra
NEXT STEPS
  • Study the properties of symmetric matrices in detail
  • Explore the implications of irreducibility in matrix theory
  • Learn about the Jordan canonical form and its applications in eigenvalue problems
  • Investigate upper Hessenberg matrices and their eigenvalue characteristics
USEFUL FOR

Mathematicians, linear algebra students, and researchers focusing on matrix theory and eigenvalue analysis will benefit from this discussion.

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Homework Statement


A) Let A be a symmetric, irreducible, tridiagonal matrix. Show that A cannot have a multiple eigenvalue.
B) Let A be an upper Hessenberg matrix with all its subdiagonal elements non-zero. Assume A has a multiple eigenvalue. Show that there can only be one eigenvector associated with it.



2. Relevant definitions
Symmetric: A = AT
Irreducible: not a good definition for it, but essentially it's well-connected
Tridiagonal: obvious
Upper Hessenberg: http://en.wikipedia.org/wiki/Hessenberg_matrix Essentially, it's a mix between a tridiagonal and a upper triangular. It's tridiagonal with non-zero elements above its 3rd subdiagonal.



The Attempt at a Solution


A) It seems contradiction would be the best combined with using the Jordan canonical form of A-\lambdaI.
Jordan canonical form: http://en.wikipedia.org/wiki/Jordan_normal_form
So, we know that we can get the Jordan canonical form of A which has all \lambda's in the diagonal.
Thus, is there anyway we can look at the canonical form of A-\lambdaI and deduce from it's rank that it has no multiple eigenvalues?
B) The hint says to use a similar strategy as A
 
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