- Art Gallery -


In linear algebra, a Jordan normal form (often called Jordan canonical form)[1] of a linear operator on a finite-dimensional vector space is an upper triangular matrix of a particular form called a Jordan matrix, representing the operator with respect to some basis. Such matrix has each non-zero off-diagonal entry equal to 1, immediately above the main diagonal (on the superdiagonal), and with identical diagonal entries to the left and below them. If the vector space is over a field K, then a basis with respect to which the matrix has the required form exists if and only if all eigenvalues of the matrix lie in K, or equivalently if the characteristic polynomial of the operator splits into linear factors over K. This condition is always satisfied if K is the field of complex numbers. The diagonal entries of the normal form are the eigenvalues of the operator, with the number of times each one occurs being given by its algebraic multiplicity.[2][3][4]

If the operator is originally given by a square matrix M, then its Jordan normal form is also called the Jordan normal form of M. Any square matrix has a Jordan normal form if the field of coefficients is extended to one containing all the eigenvalues of the matrix. In spite of its name, the normal form for a given M is not entirely unique, as it is a block diagonal matrix formed of Jordan blocks, the order of which is not fixed; it is conventional to group blocks for the same eigenvalue together, but no ordering is imposed among the eigenvalues, nor among the blocks for a given eigenvalue, although the latter could for instance be ordered by weakly decreasing size.[2][3][4]

The Jordan–Chevalley decomposition is particularly simple with respect to a basis for which the operator takes its Jordan normal form. The diagonal form for diagonalizable matrices, for instance normal matrices, is a special case of the Jordan normal form.[5][6][7]

The Jordan normal form is named after Camille Jordan.


Some textbooks have the ones on the subdiagonal, i.e., immediately below the main diagonal instead of on the superdiagonal. The eigenvalues are still on the main diagonal.[8][9]

An n × n matrix A is diagonalizable if and only if the sum of the dimensions of the eigenspaces is n. Or, equivalently, if and only if A has n linearly independent eigenvectors. Not all matrices are diagonalizable. Consider the following matrix:

\( A= \left[\!\!\!\begin{array}{*{20}{r}} 5 & 4 & 2 & 1 \\[2pt] 0 & 1 & -1 & -1 \\[2pt] -1 & -1 & 3 & 0 \\[2pt] 1 & 1 & -1 & 2 \end{array}\!\!\right]. \)

Including multiplicity, the eigenvalues of A are λ = 1, 2, 4, 4. The dimension of the kernel of (A − 4In) is 1 (and not 2), so A is not diagonalizable. However, there is an invertible matrix P such that A = PJP−1, where

\( J = \begin{bmatrix} 1 & 0 & 0 & 0 \\[2pt] 0 & 2 & 0 & 0 \\[2pt] 0 & 0 & 4 & 1 \\[2pt] 0 & 0 & 0 & 4 \end{bmatrix}.\)

The matrix J is almost diagonal. This is the Jordan normal form of A. The section Example below fills in the details of the computation.
Complex matrices

In general, a square complex matrix A is similar to a block diagonal matrix

\( J = \begin{bmatrix} J_1 & \; & \; \\ \; & \ddots & \; \\ \; & \; & J_p\end{bmatrix}\)

where each block Ji is a square matrix of the form

\( J_i = \begin{bmatrix} \lambda_i & 1 & \; & \; \\ \; & \lambda_i & \ddots & \; \\ \; & \; & \ddots & 1 \\ \; & \; & \; & \lambda_i \end{bmatrix}.\)

So there exists an invertible matrix P such that P−1AP = J is such that the only non-zero entries of J are on the diagonal and the superdiagonal. J is called the Jordan normal form of A. Each Ji is called a Jordan block of A. In a given Jordan block, every entry on the superdiagonal is 1.

Assuming this result, we can deduce the following properties:

  • Counting multiplicity, the eigenvalues of J, therefore A, are the diagonal entries.
  • Given an eigenvalue λi, its geometric multiplicity is the dimension of Ker(A − λi I), and it is the number of Jordan blocks corresponding to λi.[10]
  • The sum of the sizes of all Jordan blocks corresponding to an eigenvalue λi is its algebraic multiplicity.[10]
  • A is diagonalizable if and only if, for every eigenvalue λ of A, its geometric and algebraic multiplicities coincide.
  • The Jordan block corresponding to λ is of the form λ I + N, where N is a nilpotent matrix defined as Nij = δi,j−1 (where δ is the Kronecker delta). The nilpotency of N can be exploited when calculating f(A) where f is a complex analytic function. For example, in principle the Jordan form could give a closed-form expression for the exponential exp(A).
  • The number of Jordan blocks corresponding to λ of size at least j is dim Ker(A - λI)j - dim Ker(A - λI)j-1. Thus, the number of Jordan blocks of size exactly j is

\( 2 \dim \ker (A - \lambda_i I)^j - \dim \ker (A - \lambda_i I)^{j+1} - \dim \ker (A - \lambda_i I)^{j-1}\)

  • Given an eigenvalue λi, its multiplicity in the minimal polynomial is the size of its largest Jordan block.

Generalized eigenvectors
Main article: Generalized eigenvectors

Consider the matrix A from the example in the previous section. The Jordan normal form is obtained by some similarity transformation P−1AP = J, i.e.

\( \; AP = PJ.\)

Let P have column vectors pi, i = 1, ..., 4, then

\( A \begin{bmatrix} p_1 & p_2 & p_3 & p_4 \end{bmatrix} = \begin{bmatrix} p_1 & p_2 & p_3 & p_4 \end{bmatrix} \begin{bmatrix} 1 & 0 & 0 & 0 \\ 0 & 2 & 0 & 0 \\ 0 & 0 & 4 & 1 \\ 0 & 0 & 0 & 4 \end{bmatrix} = \begin{bmatrix} p_1 & 2p_2 & 4p_3 & p_3+4p_4 \end{bmatrix}.\)

We see that

\( \; (A - 1 I) p_1 = 0 \)
\( \; (A - 2 I) p_2 = 0 \)
\( \; (A - 4 I) p_3 = 0 \)
\( \; (A - 4 I) p_4 = p_3. \)

For i = 1,2,3 we have \( p_i \in \operatorname{Ker}(A-\lambda_{i} I)\), i.e. pi is an eigenvector of A corresponding to the eigenvalue λi. For i=4, multiplying both sides by (A-4I) gives

\( \; (A-4I)^2 p_4 = (A-4I) p_3. \)

But \((A-4I)p_3 = 0\), so

\(\; (A-4I)^2 p_4 = 0. \)

Thus, \(p_4 \in \operatorname{Ker}(A-4 I)^2.\)

Vectors such as \(p_4 \) are called generalized eigenvectors of A.Therefore, the statement that every square matrix A can be put in Jordan normal form is equivalent to the claim that there exists a basis consisting only of eigenvectors and generalized eigenvectors of A.

Thus, given an eigenvalue λ, its corresponding Jordan block gives rise to a Jordan chain. The generator, or lead vector, say pr, of the chain is a generalized eigenvector such that (A − λ I)rpr = 0, where r is the size of the Jordan block. The vector p1 = (A − λ I)r-1pr is an eigenvector corresponding to λ. In general, pi is a preimage of pi-1 under A − λ I. So the lead vector generates the chain via multiplication by (A − λ I).

Therefore, the statement that every square matrix A can be put in Jordan normal form is equivalent to the claim that there exists a basis consisting only of eigenvectors and generalized eigenvectors of A.

A proof

We give a proof by induction. The 1 × 1 case is trivial. Let A be an n × n matrix. Take any eigenvalue λ of A. The range of A − λ I, denoted by Ran(A − λ I), is an invariant subspace of A. Also, since λ is an eigenvalue of A, the dimension Ran(A − λ I), r, is strictly less than n. Let A' denote the restriction of A to Ran(A − λ I), By inductive hypothesis, there exists a basis {p1, ..., pr} such that A' , expressed with respect to this basis, is in Jordan normal form.

Next consider the subspace Ker(A − λ I). If

\( \mathrm{Ran}(A - \lambda I) \cap \mathrm{Ker}(A - \lambda I) = \{0\},\)

the desired result follows immediately from the rank–nullity theorem. This would be the case, for example, if A was Hermitian.

Otherwise, if

\( Q = \mathrm{Ran}(A - \lambda I) \cap \mathrm{Ker}(A - \lambda I) \neq \{0\},\)

let the dimension of Q be sr. Each vector in Q is an eigenvector of A' corresponding to eigenvalue λ. So the Jordan form of A' must contain s Jordan chains corresponding to s linearly independent eigenvectors. So the basis {p1, ..., pr} must contain s vectors, say {prs+1, ..., pr}, that are lead vectors in these Jordan chains from the Jordan normal form of A'. We can "extend the chains" by taking the preimages of these lead vectors. (This is the key step of argument; in general, generalized eigenvectors need not lie in Ran(A − λ I).) Let qi be such that

\( \; (A - \lambda I) q_i = p_i \mbox{ for } i = r-s+1, \ldots, r.\)

Clearly no non-trivial linear combination of the qi can lie in Ker(A − λ I). Furthermore, no non-trivial linear combination of the qi can be in Ran(A − λ I), for that would contradict the assumption that each pi is a lead vector in a Jordan chain. The set {qi}, being preimages of the linearly independent set {pi} under A − λ I, is also linearly independent.

Finally, we can pick any linearly independent set {z1, ..., zt} that spans

\( \; \mathrm{Ker}(A - \lambda I) / Q.\)

By construction, the union the three sets {p1, ..., pr}, {q r-s+1, ..., qr}, and {z1, ..., zt} is linearly independent. Each vector in the union is either an eigenvector or a generalized eigenvector of A. Finally, by rank–nullity theorem, the cardinality of the union is n. In other words, we have found a basis that consists of eigenvectors and generalized eigenvectors of A, and this shows A can be put in Jordan normal form.


It can be shown that the Jordan normal form of a given matrix A is unique up to the order of the Jordan blocks.

Knowing the algebraic and geometric multiplicities of the eigenvalues is not sufficient to determine the Jordan normal form of A. Assuming the algebraic multiplicity m(λ) of an eigenvalue λ is known, the structure of the Jordan form can be ascertained by analyzing the ranks of the powers (A − λ I)m(λ). To see this, suppose an n × n matrix A has only one eigenvalue λ. So m(λ) = n. The smallest integer k1 such that

\( (A - \lambda I)^{k_1} = 0\)

is the size of the largest Jordan block in the Jordan form of A. (This number k1 is also called the index of λ. See discussion in a following section.) The rank of

\((A - \lambda I)^{k_1 - 1}\)

is the number of Jordan blocks of size k1. Similarly, the rank of

\( (A - \lambda I)^{k_1 - 2}\)

is twice the number of Jordan blocks of size k1 plus the number of Jordan bl Jordan structure of A. The general case is similar.

This can be used to show the uniqueness of the Jordan form. Let J1 and J2 be two Jordan normal forms of A. Then J1 and J2 are similar and have the same spectrum, including algebraic multiplicities of the eigenvalues. The procedure outlined in the previous paragraph can be used to determine the structure of these matrices. Since the rank of a matrix is preserved by similarity transformation, there is a bijection between the Jordan blocks of J1 and J2. This proves the uniqueness part of the statement.

Real matrices

If A is a real matrix, its Jordan form can still be non-real, however there exists a real invertible matrix P such that P−1AP = J is a real block diagonal matrix with each block being a real Jordan block. A real Jordan block is either identical to a complex Jordan block (if the corresponding eigenvalue \lambda_i is real), or is a block matrix itself, consisting of 2×2 blocks as follows (for non-real eigenvalue \lambda_i = a_i+ib_i). The diagonal blocks are identical, of the form

\( C_i = \begin{bmatrix} a_i & b_i \\ -b_i & a_i \\ \end{bmatrix}\)

and describe multiplication by \lambda_i in the complex plane. The superdiagonal blocks are 2×2 identity matrices. The full real Jordan block is given by

\( J_i = \begin{bmatrix} C_i & I & \; & \; \\ \; & C_i & \ddots & \; \\ \; & \; & \ddots & I \\ \; & \; & \; & C_i \\ \end{bmatrix}.\)

This real Jordan form is a consequence of the complex Jordan form. For a real matrix the nonreal eigenvectors and generalized eigenvectors can always be chosen to form complex conjugate pairs. Taking the real and imaginary part (linear combination of the vector and its conjugate), the matrix has this form with respect to the new basis.


One can see that the Jordan normal form is essentially a classification result for square matrices, and as such several important results from linear algebra can be viewed as its consequences.
Spectral mapping theorem

Using the Jordan normal form, direct calculation gives a spectral mapping theorem for the polynomial functional calculus: Let A be an n × n matrix with eigenvalues λ1, ..., λn, then for any polynomial p, p(A) has eigenvalues p1), ..., pn).

Cayley–Hamilton theorem

The Cayley–Hamilton theorem asserts that every matrix A satisfies its characteristic equation: if p is the characteristic polynomial of A, then p(A) = 0. This can be shown via direct calculation in the Jordan form, since any Jordan block for λ is annihilated by (X − λ)m where m is the multiplicity of the root λ of p, the sum of the sizes of the Jordan blocks for λ, and therefore no less than the size of the block in question. The Jordan form can be assumed to exist over a field extending the base field of the matrix, for instance over the splitting field of p; this field extension does not change the matrix p(A) in any way.

Minimal polynomial

The minimal polynomial P of a square matrix A is the unique monic polynomial of least degree, m, such that P(A) = 0. Alternatively, the set of polynomials that annihilate a given A form an ideal I in C[x], the principal ideal domain of polynomials with complex coefficients. The monic element that generates I is precisely P.

Let λ1, ..., λq be the distinct eigenvalues of A, and si be the size of the largest Jordan block corresponding to λi. It is clear from the Jordan normal form that the minimal polynomial of A has degree Σsi.

While the Jordan normal form determines the minimal polynomial, the converse is not true. This leads to the notion of elementary divisors. The elementary divisors of a square matrix A are the characteristic polynomials of its Jordan blocks. The factors of the minimal polynomial m are the elementary divisors of the largest degree corresponding to distinct eigenvalues.

The degree of an elementary divisor is the size of the corresponding Jordan block, therefore the dimension of the corresponding invariant subspace. If all elementary divisors are linear, A is diagonalizable.

Invariant subspace decompositions

The Jordan form of a n × n matrix A is block diagonal, and therefore gives a decomposition of the n dimensional Euclidean space into invariant subspaces of A. Every Jordan block Ji corresponds to an invariant subspace Xi. Symbolically, we put

\( \mathbb{C}^n = \bigoplus_{i = 1}^k X_i\)

where each Xi is the span of the corresponding Jordan chain, and k is the number of Jordan chains.

One can also obtain a slightly different decomposition via the Jordan form. Given an eigenvalue λi, the size of its largest corresponding Jordan block si is called the index of λi and denoted by ν(λi). (Therefore the degree of the minimal polynomial is the sum of all indices.) Define a subspace Yi by

\( \; Y_i = \operatorname{Ker} (\lambda_i I - A)^{\nu(\lambda_i)}.\)

This gives the decomposition

\(\mathbb{C}^n = \bigoplus_{i = 1}^l Y_i

where l is the number of distinct eigenvalues of A. Intuitively, we glob together the Jordan block invariant subspaces corresponding to the same eigenvalue. In the extreme case where A is a multiple of the identity matrix we have k = n and l = 1.

The projection onto Yi and along all the other Yj ( ji ) is called the spectral projection of A at λi and is usually denoted by Pi ; A). Spectral projections are mutually orthogonal in the sense that Pi ; A) Pj ; A) = 0 if ij. Also they commute with A and their sum is the identity matrix. Replacing every λi in the Jordan matrix J by one and zeroising all other entries gives Pi ; J), moreover if U J U−1 is the similarity transformation such that A = U J U−1 then Pi ; A) = U Pi ; J) U−1. They are not confined to finite dimensions. See below for their application to compact operators, and in holomorphic functional calculus for a more general discussion.

Comparing the two decompositions, notice that, in general, lk. When A is normal, the subspaces Xi's in the first decomposition are one-dimensional and mutually orthogonal. This is the spectral theorem for normal operators. The second decomposition generalizes more easily for general compact operators on Banach spaces.

It might be of interest here to note some properties of the index, ν(λ). More generally, for a complex number λ, its index can be defined as the least non-negative integer ν(λ) such that

\( \mathrm{Ker}(\lambda - A)^{\nu(\lambda)} = \operatorname{Ker} (\lambda - A)^m, \; \forall m \geq \nu(\lambda) .\)

So ν(λ) > 0 if and only if λ is an eigenvalue of A. In the finite-dimensional case, ν(λ) ≤ the algebraic multiplicity of λ.

Matrices with entries in a field

Jordan reduction can be extended to any square matrix M whose entries lie in a field K. The result states that any M can be written as a sum D + N where D is semisimple, N is nilpotent, and DN = ND. This is called the Jordan–Chevalley decomposition. Whenever K contains the eigenvalues of M, in particular when K is algebraically closed, the normal form can be expressed explicitly as the direct sum of Jordan blocks.

Similar to the case when K is the complex numbers, knowing the dimensions of the kernels of (M − λI)k for 1 ≤ km, where m is the algebraic multiplicity of the eigenvalue λ, allows one to determine the Jordan form of M. We may view the underlying vector space V as a K[x]-module by regarding the action of x on V as application of M and extending by K-linearity. Then the polynomials (x − λ)k are the elementary divisors of M, and the Jordan normal form is concerned with representing M in terms of blocks associated to the elementary divisors.

The proof of the Jordan normal form is usually carried out as an application to the ring K[x] of the structure theorem for finitely generated modules over a principal ideal domain, of which it is a corollary.

Compact operators

In a different direction, for compact operators on a Banach space, a result analogous to the Jordan normal form holds. One restricts to compact operators because every point x in the spectrum of a compact operator T, the only exception being when x is the limit point of the spectrum, is an eigenvalue. This is not true for bounded operators in general. To give some idea of this generalization, we first reformulate the Jordan decomposition in the language of functional analysis.

Holomorphic functional calculus
For more details on this topic, see holomorphic functional calculus.

Let X be a Banach space, L(X) be the bounded operators on X, and σ(T) denote the spectrum of T ∈ L(X). The holomorphic functional calculus is defined as follows:

Fix a bounded operator T. Consider the family Hol(T) of complex functions that is holomorphic on some open set G containing σ(T). Let Γ = {γi} be a finite collection of Jordan curves such that σ(T) lies in the inside of Γ, we define f(T) by

\( f(T) = \frac{1}{2 \pi i} \int_{\Gamma} f(z)(z - T)^{-1} dz.\)

The open set G could vary with f and need not be connected. The integral is defined as the limit of the Riemann sums, as in the scalar case. Although the integral makes sense for continuous f, we restrict to holomorphic functions to apply the machinery from classical function theory (e.g. the Cauchy integral formula). The assumption that σ(T) lie in the inside of Γ ensures f(T) is well defined; it does not depend on the choice of Γ. The functional calculus is the mapping Φ from Hol(T) to L(X) given by

\( \; \Phi(f) = f(T).\)

We will require the following properties of this functional calculus:

Φ extends the polynomial functional calculus.
The spectral mapping theorem holds: σ(f(T)) = f(σ(T)).
Φ is an algebra homomorphism.

The finite-dimensional case

In the finite-dimensional case, σ(T) = {λi} is a finite discrete set in the complex plane. Let ei be the function that is 1 in some open neighborhood of λi and 0 elsewhere. By property 3 of the functional calculus, the operator

\( \; e_i(T)\)

is a projection. Moreoever, let νi be the index of λi and

\( f(z)= (z - \lambda_i)^{\nu_i}.\)

The spectral mapping theorem tells us

\( f(T) e_i (T) = (T - \lambda_i)^{\nu_i} e_i (T)\)

has spectrum {0}. By property 1, f(T) can be directly computed in the Jordan form, and by inspection, we see that the operator f(T)ei(T) is the zero matrix.

By property 3, f(T) ei(T) = ei(T) f(T). So ei(T) is precisely the projection onto the subspace

\( \mathrm{Ran} \; e_i (T) = \mathrm{Ker}(T - \lambda_i)^{\nu_i}.\)

The relation

\( \; \sum_i e_i = 1\)


\( \mathbb{C}^n = \bigoplus_i \; \mathrm{Ran}\; e_i (T) = \bigoplus_i \; \mathrm{Ker}(T - \lambda_i)^{\nu_i}\)

where the index i runs through the distinct eigenvalues of T. This is exactly the invariant subspace decomposition

\( \mathbb{C}^n = \bigoplus_i Y_i

given in a previous section. Each ei(T) is the projection onto the subspace spanned by the Jordan chains corresponding to λi and along the subspaces spanned by the Jordan chains corresponding to λj for ji. In other words ei(T) = Pi;T). This explicit identification of the operators ei(T) in turn gives an explicit form of holomorphic functional calculus for matrices:

For all f ∈ Hol(T),

\( f(T) = \sum_{\lambda_i \in \sigma(T)} \sum_{k = 0}^{\nu_i -1} \frac{f^{(k)}}{k!} (T - \lambda_i)^k e_i (T).\)

Notice that the expression of f(T) is a finite sum because, on each neighborhood of λi, we have chosen the Taylor series expansion of f centered at λi.

Poles of an operator

Let T be a bounded operator λ be an isolated point of σ(T). (As stated above, when T is compact, every point in its spectrum is an isolated point, except possibly the limit point 0.)

The point λ is called a pole of operator T with order ν if the resolvent function RT defined by

\( \; R_T(\lambda) = (\lambda - T)^{-1}\)

has a pole of order ν at λ.

We will show that, in the finite-dimensional case, the order of an eigenvalue coincides with its index. The result also holds for compact operators.

Consider the annular region A centered at the eigenvalue λ with sufficiently small radius ε such that the intersection of the open disc Bε(λ) and σ(T) is {λ}. The resolvent function RT is holomorphic on A. Extending a result from classical function theory, RT has a Laurent series representation on A:

\( R_T(z) = \sum _{- \infty} ^{\infty} a_m (\lambda - z)^m\)


\( a_{-m} = - \frac{1}{2 \pi i} \int_C (\lambda - z) ^{m-1} (z - T)^{-1} d z\) and C is a small circle centered at λ.

By the previous discussion on the functional calculus,

\( \; a_{-m} = -(\lambda - T)^{m-1} e_{\lambda} (T) where \; e_{\lambda}\) is 1 on \( \; B_{\epsilon}(\lambda)\) and 0 elsewhere.

But we have shown that the smallest positive integer m such that

\( a_{-m} \neq 0 and a_{-l} = 0 \; \; \forall \; l \geq m \)

is precisely the index of λ, ν(λ). In other words, the function RT has a pole of order ν(λ) at λ.

This example shows how to calculate the Jordan normal form of a given matrix. As the next section explains, it is important to do the computation exactly instead of rounding the results.

Consider the matrix

\( A = \begin{bmatrix} 5 & 4 & 2 & 1 \\ 0 & 1 & -1 & -1 \\ -1 & -1 & 3 & 0 \\ 1 & 1 & -1 & 2 \end{bmatrix}\)

which is mentioned in the beginning of the article.

The characteristic polynomial of A is

\( \chi(\lambda) = \det(\lambda I - A) = \lambda^4 - 11 \lambda^3 + 42 \lambda^2 - 64 \lambda + 32 = (\lambda-1)(\lambda-2)(\lambda-4)^2. \, \)

This shows that the eigenvalues are 1, 2, 4 and 4, according to algebraic multiplicity. The eigenspace corresponding to the eigenvalue 1 can be found by solving the equation Av = λ v. It is spanned by the column vector v = (−1, 1, 0, 0)T. Similarly, the eigenspace corresponding to the eigenvalue 2 is spanned by w = (1, −1, 0, 1)T. Finally, the eigenspace corresponding to the eigenvalue 4 is also one-dimensional (even though this is a double eigenvalue) and is spanned by x = (1, 0, −1, 1)T. So, the geometric multiplicity (i.e., the dimension of the eigenspace of the given eigenvalue) of each of the three eigenvalues is one. Therefore, the two eigenvalues equal to 4 correspond to a single Jordan block, and the Jordan normal form of the matrix A is the direct sum

\( J = J_1(1) \oplus J_1(2) \oplus J_2(4) = \begin{bmatrix} 1 & 0 & 0 & 0 \\ 0 & 2 & 0 & 0 \\ 0 & 0 & 4 & 1 \\ 0 & 0 & 0 & 4 \end{bmatrix}. \)

There are three chains. Two have length one: {v} and {w}, corresponding to the eigenvalues 1 and 2, respectively. There is one chain of length two corresponding to the eigenvalue 4. To find this chain, calculate

\( \ker{(A-4I)}^2 = \operatorname{span} \, \left\{ \begin{bmatrix} 1 \\ 0 \\ 0 \\ 0 \end{bmatrix}, \begin{bmatrix} 1 \\ 0 \\ -1 \\ 1 \end{bmatrix} \right\}.\)

Pick a vector in the above span that is not in the kernel of A − 4I, e.g., y = (1,0,0,0)T. Now, (A − 4I)y = x and (A − 4I)x = 0, so {y, x} is a chain of length two corresponding to the eigenvalue 4.

The transition matrix P such that P−1AP = J is formed by putting these vectors next to each other as follows

\( P = \Big[ \,v\, \Big| \,w\, \Big| \,x\, \Big| \,y\, \Big] = \begin{bmatrix} -1 & 1 & 1 & 1 \\ 1 & -1 & 0 & 0 \\ 0 & 0 & -1 & 0 \\ 0 & 1 & 1 & 0 \end{bmatrix}. \)

A computation shows that the equation P−1AP = J indeed holds.

\( P^{-1}AP=J=\begin{bmatrix} 1 & 0 & 0 & 0 \\ 0 & 2 & 0 & 0 \\ 0 & 0 & 4 & 1 \\ 0 & 0 & 0 & 4\) \end{bmatrix}.

If we had interchanged the order of which the chain vectors appeared, that is, changing the order of v, w and {x, y} together, the Jordan blocks would be interchanged. However, the Jordan forms are equivalent Jordan forms.

Numerical analysis

If the matrix A has multiple eigenvalues, or is close to a matrix with multiple eigenvalues, then its Jordan normal form is very sensitive to perturbations. Consider for instance the matrix

\( A = \begin{bmatrix} 1 & 1 \\ \varepsilon & 1 \end{bmatrix}. \)

If ε = 0, then the Jordan normal form is simply

\( \begin{bmatrix} 1 & 1 \\ 0 & 1 \end{bmatrix}. \)

However, for ε ≠ 0, the Jordan normal form is

\( \begin{bmatrix} 1+\sqrt\varepsilon & 0 \\ 0 & 1-\sqrt\varepsilon \end{bmatrix}. \)

This ill conditioning makes it very hard to develop a robust numerical algorithm for the Jordan normal form, as the result depends critically on whether two eigenvalues are deemed to be equal. For this reason, the Jordan normal form is usually avoided in numerical analysis; the stable Schur decomposition[11] or pseudospectra[12] are better alternatives.


If n is a natural number, the nth power of a matrix in Jordan normal form will be a direct sum of upper triangular matrices, as a result of block multiplication. More specifically, after exponentiation each Jordan block will be an upper triangular block.

For example,

\( \begin{bmatrix} 2 & 1 & 0 & 0 & 0 \\ 0 & 2 & 1 & 0 & 0 \\ 0 & 0 & 2 & 0 & 0 \\ 0 & 0 & 0 & 5 & 1 \\ 0 & 0 & 0 & 0 & 5 \end{bmatrix}^4 =\begin{bmatrix} 16 & 32 & 24 & 0 & 0 \\ 0 & 16 & 32 & 0 & 0 \\ 0 & 0 & 16 & 0 & 0 \\ 0 & 0 & 0 & 625 & 500 \\ 0 & 0 & 0 & 0 & 625 \end{bmatrix}.\)

Further, each triangular block will consist of λn on the main diagonal, \( \tbinom{n}{1}\) times λn-1 on the upper diagonal, and so on. This expression is valid for negative integer powers as well if one extends the notion of the binomial coefficients \( \tbinom{n}{k}\mapsto\left(\frac{n}{|n|}\right)^k\tbinom{|n|}{k}\).

For example,

\( \begin{bmatrix} \lambda_1 & 1 & 0 & 0 & 0 \\ 0 & \lambda_1 & 1 & 0 & 0 \\ 0 & 0 & \lambda_1 & 0 & 0 \\ 0 & 0 & 0 & \lambda_2 & 1 \\ 0 & 0 & 0 & 0 & \lambda_2 \end{bmatrix}^n =\begin{bmatrix} \lambda_1^n & \tbinom{n}{1}\lambda_1^{n-1} & \tbinom{n}{2}\lambda_1^{n-2} & 0 & 0 \\ 0 & \lambda_1^n & \tbinom{n}{1}\lambda_1^{n-1} & 0 & 0 \\ 0 & 0 & \lambda_1^n & 0 & 0 \\ 0 & 0 & 0 & \lambda_2^n & \tbinom{n}{1}\lambda_2^{n-1} \\ 0 & 0 & 0 & 0 & \lambda_2^n \end{bmatrix}.\)

See also

Canonical form
Frobenius normal form
Jordan matrix
Jordan–Chevalley decomposition
Matrix decomposition
Weyr canonical form


Shilov defines the term Jordan canonical form and in a footnote says that Jordan normal form is synonymous. These terms are sometimes shortened to Jordan form. (Shilov) The term Classical canonical form is also sometimes used in the sense of this article. (James & James, 1976)
Beauregard & Fraleigh (1973, pp. 310–316)
Golub & Van Loan (1996, p. 355)
Nering (1970, pp. 118–127)
Beauregard & Fraleigh (1973, pp. 270–274)
Golub & Van Loan (1996, p. 353)
Nering (1970, pp. 113–118)
Cullen (1966, p. 114)
Franklin (1968, p. 122)
Horn & Johnson (1985, §3.2.1)
See Golub & Van Loan (2014), §7.6.5; or Golub & Wilkinson (1976) for details.

See Golub & Van Loan (2014), §7.9


Beauregard, Raymond A.; Fraleigh, John B. (1973), A First Course In Linear Algebra: with Optional Introduction to Groups, Rings, and Fields, Boston: Houghton Mifflin Co., ISBN 0-395-14017-X
Cullen, Charles G. (1966), Matrices and Linear Transformations, Reading: Addison-Wesley, LCCN 66021267
N. Dunford and J.T. Schwartz, Linear Operators, Part I: General Theory, Interscience, 1958.
Daniel T. Finkbeiner II, Introduction to Matrices and Linear Transformations, Third Edition, Freeman, 1978.
Franklin, Joel N. (1968), Matrix Theory, Englewood Cliffs: Prentice-Hall, LCCN 68016345
Gene H. Golub and Charles F. Van Loan, Matrix Computations (4th ed.), Johns Hopkins University Press, Baltimore, 2012.
Gene H. Golub and J. H. Wilkinson, Ill-conditioned eigensystems and the computation of the Jordan normal form, SIAM Review, vol. 18, nr. 4, pp. 578–619, 1976.
Horn, Roger A.; Johnson, Charles R. (1985), Matrix Analysis, Cambridge University Press, ISBN 978-0-521-38632-6.
Glenn James and Robert C. James, Mathematics Dictionary, Fourth Edition, Van Nostrand Reinhold, 1976.
Saunders MacLane and Garrett Birkhoff, Algebra, MacMillan, 1967.
Anthony N. Michel and Charles J. Herget, Applied Algebra and Functional Analysis, Dover, 1993.
Nering, Evar D. (1970), Linear Algebra and Matrix Theory (2nd ed.), New York: Wiley, LCCN 76091646
Georgi E. Shilov, Linear Algebra, Dover, 1977.
I. R. Shafarevich & A. O. Remizov (2012) Linear Algebra and Geometry, Springer ISBN 978-3-642-30993-9.
Jordan Canonical Form article at mathworld.wolfram.com

External links

On line tool on Jordan form and matrix diagonalizations by www.mathstools.com

Mathematics Encyclopedia

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