8.1. Introduction to Eigenvalues and Eigenvectors

Matrix multiplication involves a lot of stretching and rotation for a vector. When we multiply a matrix and a vector together (\(\mathbf{A}\,\bm{x}\)), the result is usually a stretching and a rotation of the original vector \(\bm{x}\). However, that is not always the case. There are special matrices that rotate a vector, but do not change its length. See Rotation of a Point for more on rotation matrices. There are also vectors corresponding to square matrices that are stretched by the multiplication, but not rotated. This latter case is what we consider here.

Consider the following matrix and three vectors.

\[\begin{split}\mathbf{A} = \begin{bmatrix} 6 & 1 \\ 8 & 4 \end{bmatrix}, \quad \bm{x}_1 = \begin{bmatrix} 1 \\ 2 \end{bmatrix}, \quad \bm{x}_2 = \begin{bmatrix} 1 \\ -4 \end{bmatrix}, \quad \bm{x}_3 = \begin{bmatrix} 1 \\ -1 \end{bmatrix}\end{split}\]
\[\begin{split}\mathbf{A}\,\bm{x}_1 = \begin{bmatrix} 8 \\ 16 \end{bmatrix} = 8\;\bm{x}_1, \quad \mathbf{A}\,\bm{x}_2 = \begin{bmatrix} 2 \\ -8 \end{bmatrix} = 2\,\bm{x}_2, \quad \mathbf{A}\,\bm{x}_3 = \begin{bmatrix} 5 \\ 4 \end{bmatrix}\end{split}\]

Fig. 8.1 shows the three vectors and the product of each vector with the \(\bf{A}\) matrix. The product \(\mathbf{A}\,\bm{x}_3\) shows the typical matrix-to-vector multiplication result. The multiplication both stretches and rotates the vector. But in the cases of \(\mathbf{A}\,\bm{x}_1\) and \(\mathbf{A}\,\bm{x}_2\), the vectors are stretched, but not rotated. This is because vectors \(\bm{x}_1\) and \(\bm{x}_2\) are eigenvectors of matrix \(\bf{A}\). The eigenvalues tell us the stretching (scaling) factor for each eigenvector.

Eigenvectors are only scaled by matrix multiplication. Other vectors are both scaled and rotated by multiplication.

Fig. 8.1 Eigenvectors are only scaled by matrix multiplication. Other vectors are both scaled and rotated by multiplication.

When a vector \(\bm{x}_i\) is one of the eigenvectors of a matrix \(\bf{A}\), the following special relationship holds.

\[\boxed{\mathbf{A}\,\bm{x}_i = \lambda_i\,\bm{x}_i}\]

The power of this relationship is that when, and only when, we multiply a matrix by one of its eigenvectors, then, in a simplified equation, we can replace the matrix with a scalar.

For the \(n{\times}n\) square matrix, there are \(n\) eigenvectors, \(\bm{x_i}\), and \(n\) corresponding scalar eigenvalues, \(\lambda_i\). Each coupled eigenvalue and eigenvector pair is called an eigenpair.