- #1
mathmari
Gold Member
MHB
- 5,049
- 7
Hey!
Let $\mathbb{K}$ be a field and let $1\leq n\in \mathbb{N}$. Let $a_0, \ldots , a_{n-1}\in \mathbb{K}$ and let $m_n\in M_n(\mathbb{K})$ be given by \begin{equation*}m_n:=\begin{pmatrix}0 & 0 & \ldots & 0 & -a_0 \\ 1 & \ddots & \ddots & \vdots & \vdots \\ 0 & \ddots & \ddots & 0 & \vdots \\ \vdots & \ddots & \ddots & 0 & \vdots \\ 0 & \ldots & 0 & 1 & -a_{n-1}\end{pmatrix}\end{equation*}
I want to show that for $\lambda\in \mathbb{K}$ it holds that $\displaystyle{\det (\lambda u_n-m_n) =\lambda^n+\sum_{i=0}^{n-1}a_i \lambda^i}$. First I applied the Laplace theorem to show that the formula bust be this one:
\begin{equation*}\det (\lambda u_n-m_n)=\begin{vmatrix}\lambda & 0 & \ldots & 0 & a_0 \\ -1 & \ddots & \ddots & \vdots & \vdots \\ 0 & \ddots & \ddots & 0 & \vdots \\ \vdots & \ddots & \ddots & \lambda & \vdots \\ 0 & \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}\end{equation*}
Laplace as for the first row:
\begin{equation*}\det (\lambda u_n-m_n)=\begin{vmatrix}\lambda & 0 & \ldots & 0 & a_0 \\ -1 & \ddots & \ddots & \vdots & \vdots \\ 0 & \ddots & \ddots & 0 & \vdots \\ \vdots & \ddots & \ddots & \lambda & \vdots \\ 0 & \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}=\lambda \begin{vmatrix} \lambda & 0 & \vdots & a_1 \\ -1 & \ddots & 0 & \vdots \\ \ddots & \ddots & \lambda & \vdots \\ \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{n+1}a_0\begin{vmatrix}-1 & \lambda & \ddots & \vdots \\ 0 & \ddots & \ddots & 0 \\ \vdots & \ddots & \ddots & \lambda \\ 0 & \ldots & 0 & -1 \end{vmatrix}\end{equation*}
The matrix $\begin{pmatrix}-1 & \lambda & \ddots & \vdots \\ 0 & \ddots & \ddots & 0 \\ \vdots & \ddots & \ddots & \lambda \\ 0 & \ldots & 0 & -1 \end{pmatrix}$ is a triangular matrix, so the determiannt is the product of the diagonal elements, i.e. $(-1)^{n-1}$.
So we get \begin{align*}\det (\lambda u_n-m_n)&=\begin{vmatrix}\lambda & 0 & \ldots & 0 & a_0 \\ -1 & \ddots & \ddots & \vdots & \vdots \\ 0 & \ddots & \ddots & 0 & \vdots \\ \vdots & \ddots & \ddots & \lambda & \vdots \\ 0 & \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix} =\lambda \begin{vmatrix} \lambda & 0 & \vdots & a_1 \\ -1 & \ddots & 0 & \vdots \\ \ddots & \ddots & \lambda & \vdots \\ \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{n+1}a_0(-1)^{n-1}\\ & =\lambda \begin{vmatrix} \lambda & 0 & \vdots & a_1 \\ -1 & \ddots & 0 & \vdots \\ \ddots & \ddots & \lambda & \vdots \\ \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{2n}a_0 =\lambda \begin{vmatrix} \lambda & 0 & \vdots & a_1 \\ -1 & \ddots & 0 & \vdots \\ \ddots & \ddots & \lambda & \vdots \\ \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+a_0\end{align*}
We expand again as for the first row:
\begin{align*}\det (\lambda u_n-m_n)&=\lambda \left (\lambda \begin{vmatrix} \lambda & 0 & a_2 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^na_1\begin{vmatrix} -1 & \ddots & 0 \\ \ddots & \ddots & \lambda \\ \ldots & 0 & -1 \end{vmatrix}\right )+a_0\\ & =\lambda \left (\lambda \begin{vmatrix} \lambda & 0 & a_2 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^na_1(-1)^{n-2}\right )+a_0 \\ & =\lambda \left (\lambda \begin{vmatrix} \lambda & 0 & a_2 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{2n-2}a_1\right )+a_0 \\ & =\lambda^2 \begin{vmatrix} \lambda & 0 & a_2 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+ a_1 \lambda+a_0\end{align*}
We expand again as for the first row:
\begin{align*}\det (\lambda u_n-m_n)&=\lambda^2 \left (\lambda \begin{vmatrix} \lambda & 0 & a_3 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{n-1}a_2\begin{vmatrix} -1 & \ddots & 0 \\ \ddots & \ddots & \lambda \\ \ldots & 0 & -1 \end{vmatrix}\right )+a_1\lambda +a_0\\ & =\lambda^2 \left (\lambda \begin{vmatrix} \lambda & 0 & a_3 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{n-1}a_2(-1)^{n-3}\right )+a_1\lambda +a_0 \\ & =\lambda^2 \left (\lambda \begin{vmatrix} \lambda & 0 & a_3 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{2n-4}a_2\right )+a_1\lambda +a_0 \\ & =\lambda^3 \begin{vmatrix} \lambda & 0 & a_3 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+a_2\lambda^2+a_1\lambda +a_0\end{align*}
If we aply the Laplace explansion several times, we see that the formula is:
\begin{equation*}\det (\lambda u_n-m_n) =\lambda^n+\sum_{i=0}^{n-1}a_i \lambda^i\end{equation*}
Now we show that this formula is true using induction. (Is the way I do that correct?)
At the base case we have $n=1$, or not? But how is the matrix for $n=1$ ? Do we have that \begin{equation*}\det (\lambda u_1-m_1)=\begin{vmatrix}\lambda \end{vmatrix}=\lambda\end{equation*} ? But then the formula wouldn't hold, would it?
:unsure:
Let $\mathbb{K}$ be a field and let $1\leq n\in \mathbb{N}$. Let $a_0, \ldots , a_{n-1}\in \mathbb{K}$ and let $m_n\in M_n(\mathbb{K})$ be given by \begin{equation*}m_n:=\begin{pmatrix}0 & 0 & \ldots & 0 & -a_0 \\ 1 & \ddots & \ddots & \vdots & \vdots \\ 0 & \ddots & \ddots & 0 & \vdots \\ \vdots & \ddots & \ddots & 0 & \vdots \\ 0 & \ldots & 0 & 1 & -a_{n-1}\end{pmatrix}\end{equation*}
I want to show that for $\lambda\in \mathbb{K}$ it holds that $\displaystyle{\det (\lambda u_n-m_n) =\lambda^n+\sum_{i=0}^{n-1}a_i \lambda^i}$. First I applied the Laplace theorem to show that the formula bust be this one:
\begin{equation*}\det (\lambda u_n-m_n)=\begin{vmatrix}\lambda & 0 & \ldots & 0 & a_0 \\ -1 & \ddots & \ddots & \vdots & \vdots \\ 0 & \ddots & \ddots & 0 & \vdots \\ \vdots & \ddots & \ddots & \lambda & \vdots \\ 0 & \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}\end{equation*}
Laplace as for the first row:
\begin{equation*}\det (\lambda u_n-m_n)=\begin{vmatrix}\lambda & 0 & \ldots & 0 & a_0 \\ -1 & \ddots & \ddots & \vdots & \vdots \\ 0 & \ddots & \ddots & 0 & \vdots \\ \vdots & \ddots & \ddots & \lambda & \vdots \\ 0 & \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}=\lambda \begin{vmatrix} \lambda & 0 & \vdots & a_1 \\ -1 & \ddots & 0 & \vdots \\ \ddots & \ddots & \lambda & \vdots \\ \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{n+1}a_0\begin{vmatrix}-1 & \lambda & \ddots & \vdots \\ 0 & \ddots & \ddots & 0 \\ \vdots & \ddots & \ddots & \lambda \\ 0 & \ldots & 0 & -1 \end{vmatrix}\end{equation*}
The matrix $\begin{pmatrix}-1 & \lambda & \ddots & \vdots \\ 0 & \ddots & \ddots & 0 \\ \vdots & \ddots & \ddots & \lambda \\ 0 & \ldots & 0 & -1 \end{pmatrix}$ is a triangular matrix, so the determiannt is the product of the diagonal elements, i.e. $(-1)^{n-1}$.
So we get \begin{align*}\det (\lambda u_n-m_n)&=\begin{vmatrix}\lambda & 0 & \ldots & 0 & a_0 \\ -1 & \ddots & \ddots & \vdots & \vdots \\ 0 & \ddots & \ddots & 0 & \vdots \\ \vdots & \ddots & \ddots & \lambda & \vdots \\ 0 & \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix} =\lambda \begin{vmatrix} \lambda & 0 & \vdots & a_1 \\ -1 & \ddots & 0 & \vdots \\ \ddots & \ddots & \lambda & \vdots \\ \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{n+1}a_0(-1)^{n-1}\\ & =\lambda \begin{vmatrix} \lambda & 0 & \vdots & a_1 \\ -1 & \ddots & 0 & \vdots \\ \ddots & \ddots & \lambda & \vdots \\ \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{2n}a_0 =\lambda \begin{vmatrix} \lambda & 0 & \vdots & a_1 \\ -1 & \ddots & 0 & \vdots \\ \ddots & \ddots & \lambda & \vdots \\ \ldots & 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+a_0\end{align*}
We expand again as for the first row:
\begin{align*}\det (\lambda u_n-m_n)&=\lambda \left (\lambda \begin{vmatrix} \lambda & 0 & a_2 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^na_1\begin{vmatrix} -1 & \ddots & 0 \\ \ddots & \ddots & \lambda \\ \ldots & 0 & -1 \end{vmatrix}\right )+a_0\\ & =\lambda \left (\lambda \begin{vmatrix} \lambda & 0 & a_2 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^na_1(-1)^{n-2}\right )+a_0 \\ & =\lambda \left (\lambda \begin{vmatrix} \lambda & 0 & a_2 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{2n-2}a_1\right )+a_0 \\ & =\lambda^2 \begin{vmatrix} \lambda & 0 & a_2 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+ a_1 \lambda+a_0\end{align*}
We expand again as for the first row:
\begin{align*}\det (\lambda u_n-m_n)&=\lambda^2 \left (\lambda \begin{vmatrix} \lambda & 0 & a_3 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{n-1}a_2\begin{vmatrix} -1 & \ddots & 0 \\ \ddots & \ddots & \lambda \\ \ldots & 0 & -1 \end{vmatrix}\right )+a_1\lambda +a_0\\ & =\lambda^2 \left (\lambda \begin{vmatrix} \lambda & 0 & a_3 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{n-1}a_2(-1)^{n-3}\right )+a_1\lambda +a_0 \\ & =\lambda^2 \left (\lambda \begin{vmatrix} \lambda & 0 & a_3 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+(-1)^{2n-4}a_2\right )+a_1\lambda +a_0 \\ & =\lambda^3 \begin{vmatrix} \lambda & 0 & a_3 \\ \ddots & \lambda & \vdots \\ 0 & -1 & \lambda+a_{n-1}\end{vmatrix}+a_2\lambda^2+a_1\lambda +a_0\end{align*}
If we aply the Laplace explansion several times, we see that the formula is:
\begin{equation*}\det (\lambda u_n-m_n) =\lambda^n+\sum_{i=0}^{n-1}a_i \lambda^i\end{equation*}
Now we show that this formula is true using induction. (Is the way I do that correct?)
At the base case we have $n=1$, or not? But how is the matrix for $n=1$ ? Do we have that \begin{equation*}\det (\lambda u_1-m_1)=\begin{vmatrix}\lambda \end{vmatrix}=\lambda\end{equation*} ? But then the formula wouldn't hold, would it?
:unsure: