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Properties of Eigenvalues and Eigenvectors

Properties

  • The eigenvalues of a triangular matrix (upper, lower, or diagonal) are the entries on its main diagonal E.g. [abc0de00f]\left[ \begin{array}{rrr} \colorTwo{a} & b & c\\ 0 & \colorTwo{d} & e\\ 0 & 0 & \colorTwo{f}\\ \end{array} \right] has eigenvalues λ1=a,λ2=d,λ3=f\lambda_1 = \colorTwo{a},\quad \lambda_2 = \colorTwo{d},\quad \lambda_3 = \colorTwo{f}
  • AA is invertible if and only if 0 is not an eigenvalue of AA
  • If x\vec x is an eigenvector of AA with eigenvalue λ\lambda, then Amx=λmxA^m\vec x = \lambda^m\vec x
Checking Eigenvalues
For any square matrix An×nA_{n \times n} with eigenvalues λ1,λ2,,λn\lambda_1, \lambda_2,\dots,\lambda_n:
  • det(A)=λ1×λ2××λn\text{det}(A)=\lambda_1\times\lambda_2 \times \ldots \times \lambda_n
  • tr(A)= a11+a22++ann=λ1+λ2 ++λn\text{tr}(A)=\ a_{11}+a_{22}+\cdots+a_{nn}=\lambda_1+\lambda_{2\ }+\ldots+\lambda_n
Wize Concept
tr(A)\text{tr}(A) is the trace of a matrix An×nA_{n \times n}, which is defined as the sum of the entries on the main diagonal.

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Similar Matrices

Given An×nA_{n \times n} and any invertible matrix PP, then we say AA is similar to P1APP^{-1}AP.
Letting B=P1APB=P^{-1}AP, then BB is similar to AA which we denote BAB \sim A.
Similar matrices have the same eigenvalues!
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Example: Similar Matrices

Suppose A=[3241]A=\begin{bmatrix}3&2\\4&1\end{bmatrix} . Consider the matrix P=12[1111]P=\dfrac{1}{\sqrt{2}}\begin{bmatrix}1&-1\\1&1\end{bmatrix}, which has inverse P1=PTP^{-1}=P^T.
Find the eigenvalues of AA using the invertible matrix PP.

We want to use the formula for similar matrices: B=P1APB=P^{-1}AP.
First, find P1P^{-1}:
P1=PT=12[1111]P^{-1} = P^T =\dfrac{1}{\sqrt{2}}\begin{bmatrix}1&1\\-1&1\end{bmatrix}
Now we can find a similar matrix using the formula:
P1AP=12[1111][3241]12[1111]=12[7311][1111]=12[10402]=[5201]=B\begin{aligned} P^{-1}AP &= \dfrac{1}{\sqrt{2}}\begin{bmatrix}1&1\\-1&1\end{bmatrix} \begin{bmatrix}3&2\\4&1\end{bmatrix} \dfrac{1}{\sqrt{2}}\begin{bmatrix}1&-1\\1&1\end{bmatrix}\\[1.5em] &=\dfrac{1}{2}\begin{bmatrix}7&3\\1&-1\end{bmatrix}\begin{bmatrix}1&-1\\1&1\end{bmatrix}\\[1.5em] &=\frac{1}{2}\begin{bmatrix}10&-4\\0&-2\end{bmatrix}\\[1.5em] &=\begin{bmatrix}5&-2\\0&-1\end{bmatrix}=B \end{aligned}
Since BB is upper triangular, its eigenvalues are on the main diagonal.
Therefore, the eigenvalues of BB are λ1=5\lambda_1 = 5 and λ2=1\lambda_2 = -1. Since ABA \sim B, these are also the eigenvalues of AA.
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Example: Eigenvectors and Linear Transformations

Let L:R3R3L:\mathbb{R}^3\to\mathbb{R}^3 be the linear transformation defined by:
L(x,y,z)=(2xy3zx+zx+y+2z)L(x,y,z) = \left( \begin{array}{c} -2x-y-3z\\ x+z\\ x+y+2z\\ \end{array} \right)

Part A)

If it is known that x=[110]\vec x= \begin{bmatrix} 1\\ -1\\ 0\\ \end{bmatrix} is an eigenvector of the transformation LL, find the vector (LLLLL)(x)(L \circ L \circ L \circ L \circ L)(\vec x).
Since LL is linear, it can be represented by a matrix AA such that L(v)=AvL(\vec v) = A\vec v.
Let's start by finding the matrix AA that induces this transformation:
L(xyz)=(2xy3zx+zx+y+2z)=(2x1y3z1x+0y+1z1x+1y+2z)=[213101112][xyz]L\left(\begin{array}{c}x\\y\\z\end{array}\right)=\left(\begin{array}{c}-2x-y-3z\\x+z\\x+y+2z\end{array}\right) =\left(\begin{array}{r}-2x-1y-3z\\ 1x+0y+1z\\1x+1y+2z\end{array}\right) =\left[\begin{array}{rrr}-2&-1&-3\\1&0&1\\1&1&2\end{array}\right]\left[\begin{array}{c}x\\y\\z\end{array}\right]
    A=[213101112]\implies A=\left[\begin{array}{rrr}-2&-1&-3\\1&0&1\\1&1&2\end{array}\right]
Since x\vec x is an eigenvector of LL, it must also be an eigenvector of AA. Let's find its eigenvalue:
L(x)=Ax=[213101112][110]=[110]=1xL(\vec x) = A\vec x = \left[\begin{array}{rrr}-2&-1&-3\\1&0&1\\1&1&2\end{array}\right] \left[\begin{array}{r}1\\-1\\0\end{array}\right] = \left[\begin{array}{r}-1\\1\\0\end{array}\right] = \textcolor{green}{\mathbf{-1}}\vec x
So x\vec x is an eigenvector with associated eigenvalue λ=1\lambda=\textcolor{green}{\mathbf{-1}}.
Then notice that the vector (LLLLL)(x)(L \circ L \circ L \circ L \circ L)(\vec x) is equivalent to A5xA^5\vec x, since applying LL five times is equivalent to multiplying by AA five times.
L(L(L(L(L(x)))))=A5xL(L(L(L(L(\vec x))))) = A^5 \vec x
and by a property of eigenvalues: A5x=λ5xA^5 \vec x = \lambda^5\vec x
Therefore:
(LLLLL)(x)=A5x=λ5x=(1)5x=x=[110]= [110] (L \circ L \circ L \circ L \circ L)(\vec x) =A^5\vec x = \lambda^5\vec x = (\textcolor{green}{\bm{-1}})^5\vec x = -\vec x = -\begin{bmatrix} 1\\ -1\\ 0\\ \end{bmatrix} = \boxed{\ \begin{bmatrix} -1\\ 1\\ 0\\ \end{bmatrix}\ }
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Part B)

Given that two eigenvalues of LL are λ1=1\lambda_1=1 and λ2=1\lambda_2 = -1, determine whether LL is invertible.
LL is invertible if AA is invertible, and AA is invertible if and only if 0 is not one of its eigenvalues.
The question tells us A=[213101112]A=\left[\begin{array}{rrr}-2&-1&-3\\1&0&1\\1&1&2\end{array}\right] has eigenvalues λ1=1\lambda_1=1 and λ2=1\lambda_2=-1 (since AA and LL must have the same eigenvalues).
From the properties of eigenvalues, the sum of the eigenvalues must equal the trace of matrix AA. In other words:
λ1+λ2+λ3=a11+a22+a331+(1)+λ3=(2)+0+2λ3=0\begin{aligned} \lambda_1+\lambda_2+\lambda_3 &=a_{11}+a_{22}+a_{33}\\[0.5em] 1+(-1)+\lambda_3 &=(-2)+0+2\\[0.5em] \lambda_3&=0 \end{aligned}
The third eigenvalue of AA is 0, so AA is not invertible, therefore LL is not invertible.

Practice: Similar Matrices

Consider the matrix A=[1421]A= \left[ \begin{array}{rrr} -1 & 4\\ 2 & 1 \end{array} \right].
Use the invertible matrix P=[1101]P= \left[ \begin{array}{rrr} 1 & 1\\ 0 & 1 \end{array} \right] to find a matrix similar to AA.
Extra Practice