Prerequisites:
\lambda spans a subspace, which is called the Eigenspace of A with respect to \lambda and is denoted by E_\lambda . The set of all eigenvalues of A is called Eigenspectrum, or just spectrum, of A.
If \lambda is an eigenvalue of A, then the corresponding eigenspace E_\lambda is the solution space of the homogeneous system of linear equations (A-\lambda I)x = 0 . Geometrically, the eigenvector corresponding to a non - zero eigenvalue points in a direction that is stretched by the linear mapping. The eigenvalue is the factor by which it is stretched. If the eigenvalue is negative, then the direction of the stretching is flipped.
Below are some useful properties of eigenvalues and eigenvectors in addition to the properties which are already listed in the article Mathematics | Eigen Values and Eigen Vectors.
A matrix A and its transpose A^{T} possess the same eigenvalues but not necessarily the same eigenvectors.
The eigenspace E_\lambda is the null space of A - \lambda I since
Ax = \lambda x \Longleftrightarrow Ax - \lambda x = 0 \Longleftrightarrow (A - \lambda I)x = 0 \Longleftrightarrow x\in ker(A - \lambda I)
Note: ker stands for Kernel which is another name for null space.
Computing Eigenvalues, Eigenvectors, and Eigenspaces:
E_5 and E_2 in the above example are one dimensional as they are each spanned by a single vector. However, in other cases, we may have multiple identical eigenvectors and the eigenspaces may have more than one dimension.
- Mathematics | Eigen Values and Eigen Vectors
- Matrix Multiplication
- Null Space and Nullity of a Matrix
Consider given 2 X 2 matrix:The two eigenspacesA = \begin{bmatrix} 4 & 2 \\ 1 & 3 \end{bmatrix} Step 1: Characteristic polynomial and Eigenvalues. The characteristic polynomial is given by det(A - \lambda I )= det(\begin{bmatrix} 4 & 2 \\ 1 & 3 \end{bmatrix} - \begin{bmatrix} \lambda & 0 \\ 0 & \lambda \end{bmatrix}) = \begin{vmatrix} 4-\lambda & 2 \\ 1 & 3-\lambda \end{vmatrix} = (4-\lambda)(3-\lambda) - 2.1 After we factorize the characteristic polynomial, we will get(2-\lambda)(5-\lambda) which gives eigenvalues as\lambda_1 = 2 and\lambda_2 = 5 Step 2: Eigenvectors and Eigenspaces We find the eigenvectors that correspond to these eigenvalues by looking at vectors x such that\begin{bmatrix} 4-\lambda & 2 \\ 1 & 3-\lambda \end{bmatrix} % x = 0 For\lambda = 5 we obtain\begin{bmatrix} 4-5 & 2 \\ 1 & 3-5 \end{bmatrix} % \begin{bmatrix} x_1 \\ x_2 \end{bmatrix} = \begin{bmatrix} -1 & 2 \\ 1 & -2 \end{bmatrix} % \begin{bmatrix} x_1 \\ x_2 \end{bmatrix} = 0 After solving the above homogeneous system of equations, we will obtain a solution spaceE_5 = span(\begin{bmatrix} 2 \\ 1 \end{bmatrix}) This eigenspace is one dimensional as it possesses a single basis vector. Similarly, we find eigenvector for\lambda = 2 by solving the homogeneous system of equations\begin{bmatrix} 4-2 & 2 \\ 1 & 3-2 \end{bmatrix} % \begin{bmatrix} x_1 \\ x_2 \end{bmatrix} = \begin{bmatrix} 2 & 2 \\ 1 & 1 \end{bmatrix} % \begin{bmatrix} x_1 \\ x_2 \end{bmatrix} = 0 This means any vectorx = \begin{bmatrix} x_1 \\ x_2 \end{bmatrix} , wherex_2=-x_1 such as\begin{bmatrix} 1 \\ -1 \end{bmatrix} is an eigenvector with eigenvalue 2. This means eigenspace is given asE_2 = span(\begin{bmatrix} 1 \\ -1 \end{bmatrix})