In terms of Jordan Canonical Form, and more specifically about Jordan Blocks. When there is a definition about Jordan Blocks they say the eigenvalues go on the principle diagonal and the diagonal above it(usually called the super-diagonal) contains the number 1!

I want to understand why there are 1's in the superdiagonal. I have looked all over and no body tries to explain why there is this mysterious 1's in the super-diagonal.

I hope that someone here on this forum can explain this.

Here is a link to PDF: http://ckottke.ncf.edu/docs/jordan.pdf

  • $\begingroup$ "I have looked all over": Have you looked at a proof that every (complex) matrix has a Jordan form? $\endgroup$ – David C. Ullrich Dec 22 '18 at 16:03
  • $\begingroup$ Hi David, i have seen things about complex matrix has Jordan form, but when they discuss it they assume the Ones on the Super Diagonal as though this is a fundamental axiom without need of explanation. $\endgroup$ – Palu Dec 22 '18 at 19:57
  • $\begingroup$ I just added a link to a pdf article I want to illustrate, how they explain things, where they just assume it to be a fact. See above. $\endgroup$ – Palu Dec 22 '18 at 20:00

If you have a non-zero vector $x$ such that $(A-\lambda I)^{n-1}x \ne 0$ and $(A-\lambda I)^{n}x=0$, then $$ \{x,(A-\lambda I)x,\cdots,(A-\lambda I)^{n-1}x\} $$ is a linearly independent set of vectors. Let \begin{align} v_1 & = (A-\lambda I)^{n-1}x,\\v_2 & =(A-\lambda I)^{n-2}x,\\&\cdots\\v_{n-1} & =(A-\lambda I)^{1}x\end{align}

Then $A-\lambda I$ has the following matrix representation with respect to this basis: $$ \left[\begin{array}{cccc}0 & 1 & 0 & \cdots & 0 \\ 0 & 0 & 1 & \cdots & 0\\ \vdots & \vdots & \vdots & \ddots & \vdots \\ 0 & 0 & 0 & \cdots & 1 \\ 0 & 0 & 0 & \cdots & 0 \end{array}\right] $$ And $A-\lambda I$ has the representation $\lambda I$ plus the above, which is a Jordan block. $$ \left[\begin{array}{cccc}\lambda & 1 & 0 & \cdots & 0 \\ 0 & \lambda & 1 & \cdots & 0\\ \vdots & \vdots & \vdots & \ddots & \vdots \\ 0 & 0 & \lambda & \cdots & 1 \\ 0 & 0 & 0 & \cdots & \lambda \end{array}\right] $$ So the answer to your question is that you can always choose the basis so that you get $1$'s on the diagonal above the main diagonal for a Jordan block.

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  • $\begingroup$ Hi DisintegratingByParts, i like what you have done here. When you talk about "Then A−λI has the following matrix representation with respect to this basis: " and you get that matrix that has the ones in the SuperDiagonal, i need to try to look at this more carefully, it does not jump out immediately to me. I will try to look at this carefully. Thanks for what you have provided, it looks really interesting. $\endgroup$ – Palu Dec 23 '18 at 22:03
  • $\begingroup$ Hi DisintegratingByParts, I am having difficulty with the algebra manipulation of the e basis vectors. Is e1, e2, e3 etc going to be the column vectors of the Matrix, then would i factor out the A−λI with power out. Hope you can help with this. $\endgroup$ – Palu Dec 24 '18 at 0:43
  • $\begingroup$ By a change of basis, the k-th basis element becomes $e_k$. Jordan form is achieved by a change of basis $\endgroup$ – Disintegrating By Parts Dec 24 '18 at 2:49
  • $\begingroup$ So when you use $e_k$ i guess you mean they are the standard basis of $R^n$. For example (1,0,0) , (0,1,0) and (0,0,1) for $R^3$. $\endgroup$ – Palu Dec 24 '18 at 16:07

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