Any nontrivial Jordan block of size 2 × 2 {\displaystyle 2\times 2} or larger (that is, not completely diagonal) is defective. (A diagonal matrix is a special case of the Jordan normal form with all trivial Jordan blocks of size 1 × 1 {\displaystyle 1\times 1} and is not defective.) For example, the n × n {\displaystyle n\times n} Jordan block
has an eigenvalue, λ {\displaystyle \lambda } with algebraic multiplicity n {\displaystyle n} (or greater if there are other Jordan blocks with the same eigenvalue), but only one distinct eigenvector J v 1 = λ v 1 {\displaystyle Jv_{1}=\lambda v_{1}} , where v 1 = [ 1 0 ⋮ 0 ] . {\displaystyle v_{1}={\begin{bmatrix}1\\0\\\vdots \\0\end{bmatrix}}.} The other canonical basis vectors v 2 = [ 0 1 ⋮ 0 ] , … , v n = [ 0 0 ⋮ 1 ] {\displaystyle v_{2}={\begin{bmatrix}0\\1\\\vdots \\0\end{bmatrix}},~\ldots ,~v_{n}={\begin{bmatrix}0\\0\\\vdots \\1\end{bmatrix}}} form a chain of generalized eigenvectors such that J v k = λ v k + v k − 1 {\displaystyle Jv_{k}=\lambda v_{k}+v_{k-1}} for k = 2 , … , n {\displaystyle k=2,\ldots ,n} .
Any defective matrix has a nontrivial Jordan normal form, which is as close as one can come to diagonalization of such a matrix.
A simple example of a defective matrix is
which has a double eigenvalue of 3 but only one distinct eigenvector
(and constant multiples thereof).
Golub & Van Loan (1996, p. 316) - Golub, Gene H.; Van Loan, Charles F. (1996), Matrix Computations (3rd ed.), Baltimore: Johns Hopkins University Press, ISBN 978-0-8018-5414-9 ↩