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Section 32.5 Examples

Example 32.5.1. Putting a nilpotent matrix into elementary nilpotent form.

Here we will apply Procedure 32.4.2 to the matrix

\begin{equation*} A = \left[\begin{array}{rrrr} 1 \amp 2 \amp 0 \amp -1 \\ 3 \amp 7 \amp -1 \amp -4 \\ -1 \amp 9 \amp -2 \amp -4 \\ 6 \amp 10 \amp -1 \amp -6 \end{array}\right]\text{.} \end{equation*}

Compute the powers of \(A\text{:}\)

\begin{align*} A^2 \amp = \left[\begin{array}{ccrr} 1 \amp 6 \amp -1 \amp -3 \\ 1 \amp 6 \amp -1 \amp -3 \\ 4 \amp 3 \amp -1 \amp -3 \\ 1 \amp 13 \amp -2 \amp -6 \end{array}\right] \text{,} \amp A^3 \amp = \left[\begin{array}{rrrr} 2 \amp 5 \amp -1 \amp -3 \\ 2 \amp 5 \amp -1 \amp -3 \\ -4 \amp -10 \amp 2 \amp 6 \\ 6 \amp 15 \amp -3 \amp -9 \end{array}\right] \text{,} \amp A^4 \amp = \zerovec \text{.} \end{align*}

Since every column of \(A^3\) is nonzero, we can choose \(\uvec{v}\) to be any of the standard basis vectors. Let's choose \(\uvec{v} = \uvec{e}_1\text{.}\) Then, using

\begin{align*} \uvec{p}_1 \amp= \uvec{v} = \begin{bmatrix} 1 \\ 0 \\ 0 \\ 0 \end{bmatrix} \text{,} \amp \uvec{p}_2 \amp= A\uvec{v} = \left[\begin{array}{r} 1 \\ 3 \\ -1 \\ 6 \end{array}\right] \text{,} \amp \uvec{p}_3 \amp= A^2 \uvec{v} = \begin{bmatrix} 1 \\ 1 \\ 4 \\ 1 \end{bmatrix} \text{,} \amp \uvec{p}_4 \amp= A^3 \uvec{v} = \left[\begin{array}{r} 2 \\ 2 \\ -4 \\ 6 \end{array}\right] \text{,} \end{align*}

we get

\begin{equation*} P = \left[\begin{array}{crcr} 1 \amp 1 \amp 1 \amp 2 \\ 0 \amp 3 \amp 1 \amp 2 \\ 0 \amp -1 \amp 4 \amp -4 \\ 0 \amp 6 \amp 1 \amp 6 \end{array}\right]\text{.} \end{equation*}

Because of our choice of \(\uvec{v} = \uvec{e}_1\text{,}\) there wasn't any need to actually compute the products \(A^j \uvec{v}\) to obtain the columns of \(P\text{,}\) as \(A^j \uvec{e}_1\) is just the first column of \(A^j\text{.}\)

There also isn't any need to compute \(\inv{P} A P\text{,}\) as we know our procedure will result in elementary nilpotent form

\begin{equation*} \inv{P}AP = \begin{bmatrix} 0 \amp 0 \amp 0 \amp 0 \\ 1 \amp 0 \amp 0 \amp 0 \\ 0 \amp 1 \amp 0 \amp 0 \\ 0 \amp 0 \amp 1 \amp 0 \end{bmatrix}\text{.} \end{equation*}