In linear algebra, a nilpotent matrix is a square matrix N such that
for some positive
integer . The smallest such
is called the
index of
,
sometimes the
degree of
.
More generally, a nilpotent transformation is a linear transformation of a vector space such that for some positive integer (and thus, for all ). Both of these concepts are special cases of a more general concept of nilpotent that applies to elements of rings.
Examples
Example 1
The matrix
A = \begin{bmatrix}
0 & 1 \\
0 & 0
\end{bmatrix}
is nilpotent with index 2, since
.
Example 2
More generally, any
-dimensional triangular matrix with zeros along the
main diagonal is nilpotent, with index
. For example, the matrix
B=\begin{bmatrix}
0 & 2 & 1 & 6\\
0 & 0 & 1 & 2\\
0 & 0 & 0 & 3\\
0 & 0 & 0 & 0
\end{bmatrix}
is nilpotent, with
B^2=\begin{bmatrix}
0 & 0 & 2 & 7\\
0 & 0 & 0 & 3\\
0 & 0 & 0 & 0\\
0 & 0 & 0 & 0
\end{bmatrix}
- \
B^3=\begin{bmatrix}
0 & 0 & 0 & 6\\
0 & 0 & 0 & 0\\
0 & 0 & 0 & 0\\
0 & 0 & 0 & 0
\end{bmatrix}
- \
B^4=\begin{bmatrix}
0 & 0 & 0 & 0\\
0 & 0 & 0 & 0\\
0 & 0 & 0 & 0\\
0 & 0 & 0 & 0
\end{bmatrix}
The index of is therefore 4.
Example 3
Although the examples above have a large number of zero entries, a typical nilpotent matrix does not. For example,
C=\begin{bmatrix}
5 & -3 & 2 \\
15 & -9 & 6 \\
10 & -6 & 4
\end{bmatrix}
\qquad
C^2=\begin{bmatrix}
0 & 0 & 0 \\
0 & 0 & 0 \\
0 & 0 & 0
\end{bmatrix}
although the matrix has no zero entries.
Example 4
Additionally, any matrices of the form
\begin{bmatrix}
a_1 & a_1 & \cdots & a_1 \\
a_2 & a_2 & \cdots & a_2 \\
\vdots & \vdots & \ddots & \vdots \\
-a_1-a_2-\ldots-a_{n-1} & -a_1-a_2-\ldots-a_{n-1} & \ldots & -a_1-a_2-\ldots-a_{n-1}
\end{bmatrix}
such as
\begin{bmatrix}
5 & 5 & 5 \\
6 & 6 & 6 \\
-11 & -11 & -11
\end{bmatrix}
or
1 & 1 & 1 & 1 \\
2 & 2 & 2 & 2 \\
4 & 4 & 4 & 4 \\
-7 & -7 & -7 & -7
\end{bmatrix}
square to zero.
Example 5
Perhaps some of the most striking examples of nilpotent matrices are
square matrices of the form:
2 & 2 & 2 & \cdots & 1-n \\
n+2 & 1 & 1 & \cdots & -n \\
1 & n+2 & 1 & \cdots & -n \\
1 & 1 & n+2 & \cdots & -n \\
\vdots & \vdots & \vdots & \ddots & \vdots
\end{bmatrix}
The first few of which are:
2 & -1 \\
4 & -2
\end{bmatrix}
\qquad
\begin{bmatrix}
2 & 2 & -2 \\
5 & 1 & -3 \\
1 & 5 & -3
\end{bmatrix}
\qquad
\begin{bmatrix}
2 & 2 & 2 & -3 \\
6 & 1 & 1 & -4 \\
1 & 6 & 1 & -4 \\
1 & 1 & 6 & -4
\end{bmatrix}
\qquad
\begin{bmatrix}
2 & 2 & 2 & 2 & -4 \\
7 & 1 & 1 & 1 & -5 \\
1 & 7 & 1 & 1 & -5 \\
1 & 1 & 7 & 1 & -5 \\
1 & 1 & 1 & 7 & -5
\end{bmatrix}
\qquad
\ldots
These matrices are nilpotent but there are no zero entries in any powers of them less than the index.
Example 6
Consider the linear space of
of a bounded degree. The
derivative operator is a linear map. We know that applying the derivative to a polynomial decreases its degree by one, so when applying it iteratively, we will eventually obtain zero. Therefore, on such a space, the derivative is representable by a nilpotent matrix.
Characterization
For an
square matrix
with
real number (or
complex number) entries, the following are equivalent:
-
is nilpotent.
-
The characteristic polynomial for is .
-
The minimal polynomial for is for some positive integer .
-
The only complex eigenvalue for is 0.
The last theorem holds true for matrices over any field of characteristic 0 or sufficiently large characteristic. (cf. Newton's identities)
This theorem has several consequences, including:
-
The index of an nilpotent matrix is always less than or equal to . For example, every nilpotent matrix squares to zero.
-
The determinant and trace of a nilpotent matrix are always zero. Consequently, a nilpotent matrix cannot be invertible.
-
The only nilpotent diagonalizable matrix is the zero matrix.
See also: Jordan–Chevalley decomposition#Nilpotency criterion.
Classification
Consider the
(upper)
shift matrix:
0 & 1 & 0 & \ldots & 0 \\
0 & 0 & 1 & \ldots & 0 \\
\vdots & \vdots & \vdots & \ddots & \vdots \\
0 & 0 & 0 & \ldots & 1 \\
0 & 0 & 0 & \ldots & 0
\end{bmatrix}.
This matrix has 1s along the
superdiagonal and 0s everywhere else. As a linear transformation, the shift matrix "shifts" the components of a vector one position to the left, with a zero appearing in the last position:
This matrix is nilpotent with degree
, and is the
Canonical form nilpotent matrix.
Specifically, if is any nilpotent matrix, then is similar to a block diagonal matrix of the form
S_1 & 0 & \ldots & 0 \\
0 & S_2 & \ldots & 0 \\
\vdots & \vdots & \ddots & \vdots \\
0 & 0 & \ldots & S_r
\end{bmatrix}
where each of the blocks
is a shift matrix (possibly of different sizes). This form is a special case of the Jordan canonical form for matrices.
For example, any nonzero 2 × 2 nilpotent matrix is similar to the matrix
0 & 1 \\
0 & 0
\end{bmatrix}.
That is, if
is any nonzero 2 × 2 nilpotent matrix, then there exists a basis
b1,
b2 such that
N b 1 = 0 and Nb2 =
b1.
This classification theorem holds for matrices over any field. (It is not necessary for the field to be algebraically closed.)
Flag of subspaces
A nilpotent transformation
on
naturally determines a flag of subspaces
and a signature
The signature characterizes up to an invertible linear transformation. Furthermore, it satisfies the inequalities
Conversely, any sequence of natural numbers satisfying these inequalities is the signature of a nilpotent transformation.
Additional properties
Generalizations
A
linear operator is
locally nilpotent if for every vector
, there exists a
such that
For operators on a finite-dimensional vector space, local nilpotence is equivalent to nilpotence.
Notes
External links