Kernel (linear algebra)

Kernel (linear algebra)
In mathematics, the kernel of a linear map, also known as the null space or nullspace, is the linear subspace of the domain of the map which is mapped to the zero vector. That is, given a linear map between two vector spaces and , the kernel of is the vector space of all elements of such that , where denotes the zero vector in , or more symbolically:
Properties
The kernel of is a linear subspace of the domain .
In the linear map two elements of have the same image in if and only if their difference lies in the kernel of , that is,
From this, it follows that the image of is isomorphic to the quotient of by the kernel:
In the case where is finite-dimensional, this implies the rank–nullity theorem:
where the term refers the dimension of the image of , while refers to the dimension of the kernel of ,
That is,
so that the rank–nullity theorem can be restated as
When is an inner product space, the quotient can be identified with the orthogonal complement in of This is the generalization to linear operators of the row space, or coimage, of a matrix.
Application to modules
The notion of kernel also makes sense for homomorphisms of modules, which are generalizations of vector spaces where the scalars are elements of a ring, rather than a field. The domain of the mapping is a module, with the kernel constituting a submodule. Here, the concepts of rank and nullity do not necessarily apply.
In functional analysis
If V and W are topological vector spaces such that W is finite-dimensional, then a linear operator L: V → W is continuous if and only if the kernel of L is a closed subspace of V.
Representation as matrix multiplication
Consider a linear map represented as a m × n matrix A with coefficients in a field K (typically or ), that is operating on column vectors x with n components over K.
The kernel of this linear map is the set of solutions to the equation , where 0 is understood as the zero vector. The dimension of the kernel of A is called the nullity of A. In set-builder notation,
The matrix equation is equivalent to a homogeneous system of linear equations:
Thus the kernel of A is the same as the solution set to the above homogeneous equations.
Subspace properties
The kernel of a matrix A over a field K is a linear subspace of Kn. That is, the kernel of A, the set Null(A), has the following three properties:
Null(A) always contains the zero vector, since .
If and , then . This follows from the distributivity of matrix multiplication over addition.
If and c is a scalar , then , since .
The row space of a matrix
The product Ax can be written in terms of the dot product of vectors as follows:
Here, a1, ... , am denote the rows of the matrix A. It follows that x is in the kernel of A, if and only if x is orthogonal (or perpendicular) to each of the row vectors of A (since orthogonality is defined as having a dot product of 0).
The row space, or coimage, of a matrix A is the span of the row vectors of A. By the above reasoning, the kernel of A is the orthogonal complement to the row space. That is, a vector x lies in the kernel of A, if and only if it is perpendicular to every vector in the row space of A.
The dimension of the row space of A is called the rank of A, and the dimension of the kernel of A is called the nullity of A. These quantities are related by the rank–nullity theorem
Left null space
The left null space, or cokernel, of a matrix A consists of all column vectors x such that xTA = 0T, where T denotes the transpose of a matrix. The left null space of A is the same as the kernel of AT. The left null space of A is the orthogonal complement to the column space of A, and is dual to the cokernel of the associated linear transformation. The kernel, the row space, the column space, and the left null space of A are the four fundamental subspaces associated to the matrix A.
Nonhomogeneous systems of linear equations
The kernel also plays a role in the solution to a nonhomogeneous system of linear equations:
If u and v are two possible solutions to the above equation, then
Thus, the difference of any two solutions to the equation Ax = b lies in the kernel of A.
It follows that any solution to the equation Ax = b can be expressed as the sum of a fixed solution v and an arbitrary element of the kernel. That is, the solution set to the equation Ax = b is
Geometrically, this says that the solution set to Ax = b is the translation of the kernel of A by the vector v. See also Fredholm alternative and flat (geometry).
Illustration
The following is a simple illustration of the computation of the kernel of a matrix (see , below for methods better suited to more complex calculations). The illustration also touches on the row space and its relation to the kernel.
Consider the matrix
The kernel of this matrix consists of all vectors for which
which can be expressed as a homogeneous system of linear equations involving x, y, and z:
The same linear equations can also be written in matrix form as:
Through Gauss–Jordan elimination, the matrix can be reduced to:
Rewriting the matrix in equation form yields:
The elements of the kernel can be further expressed in parametric vector form, as follows:
Since c is a free variable ranging over all real numbers, this can be expressed equally well as:
The kernel of A is precisely the solution set to these equations (in this case, a line through the origin in R3). Here, since the vector (−1,−26,16)T constitutes a basis of the kernel of A. The nullity of A is 1.
The following dot products are zero:
which illustrates that vectors in the kernel of A are orthogonal to each of the row vectors of A.
These two (linearly independent) row vectors span the row space of A—a plane orthogonal to the vector (−1,−26,16)T.
With the rank 2 of A, the nullity 1 of A, and the dimension 3 of A, we have an illustration of the rank-nullity theorem.
Examples
If , then the kernel of L is the solution set to a homogeneous system of linear equations. As in the above illustration, if L is the operator: then the kernel of L is the set of solutions to the equations
Let C[0,1] denote the vector space of all continuous real-valued functions on the interval [0,1], and define by the rule Then the kernel of L consists of all functions for which .
Let C∞(R) be the vector space of all infinitely differentiable functions , and let be the differentiation operator: Then the kernel of D consists of all functions in whose derivatives are zero, i.e. the set of all constant functions.
Let be the direct product of infinitely many copies of , and let be the shift operator Then the kernel of s is the one-dimensional subspace consisting of all vectors .
If is an inner product space and is a subspace, the kernel of the orthogonal projection is the orthogonal complement to in .
Computation by Gaussian elimination
A basis of the kernel of a matrix may be computed by Gaussian elimination.
For this purpose, given an m × n matrix A, we construct first the row augmented matrix where is the n × n identity matrix.
Computing its column echelon form by Gaussian elimination (or any other suitable method), we get a matrix A basis of the kernel of A consists in the non-zero columns of C such that the corresponding column of B is a zero column.
In fact, the computation may be stopped as soon as the upper matrix is in column echelon form: the remainder of the computation consists in changing the basis of the vector space generated by the columns whose upper part is zero.
For example, suppose that
Then
Putting the upper part in column echelon form by column operations on the whole matrix gives
The last three columns of B are zero columns. Therefore, the three last vectors of C,
are a basis of the kernel of A.
Proof that the method computes the kernel: Since column operations correspond to post-multiplication by invertible matrices, the fact that reduces to means that there exists an invertible matrix such that with in column echelon form. Thus and A column vector belongs to the kernel of (that is ) if and only if where As is in column echelon form, if and only if the nonzero entries of correspond to the zero columns of By multiplying by , one may deduce that this is the case if and only if is a linear combination of the corresponding columns of
Numerical computation
The problem of computing the kernel on a computer depends on the nature of the coefficients.
Exact coefficients
If the coefficients of the matrix are exactly given numbers, the column echelon form of the matrix may be computed by Bareiss algorithm more efficiently than with Gaussian elimination. It is even more efficient to use modular arithmetic and Chinese remainder theorem, which reduces the problem to several similar ones over finite fields (this avoids the overhead induced by the non-linearity of the computational complexity of integer multiplication).
For coefficients in a finite field, Gaussian elimination works well, but for the large matrices that occur in cryptography and Gröbner basis computation, better algorithms are known, which have roughly the same computational complexity, but are faster and behave better with modern computer hardware.
Floating point computation
For matrices whose entries are floating-point numbers, the problem of computing the kernel makes sense only for matrices such that the number of rows is equal to their rank: because of the rounding errors, a floating-point matrix has almost always a full rank, even when it is an approximation of a matrix of a much smaller rank. Even for a full-rank matrix, it is possible to compute its kernel only if it is well conditioned, i.e. it has a low condition number.
Even for a well conditioned full rank matrix, Gaussian elimination does not behave correctly: it introduces rounding errors that are too large for getting a significant result. As the computation of the kernel of a matrix is a special instance of solving a homogeneous system of linear equations, the kernel may be computed by any of the various algorithms designed to solve homogeneous systems. A state of the art software for this purpose is the Lapack library.
See also
Kernel (algebra)
Zero set
System of linear equations
Row and column spaces
Row reduction
Four fundamental subspaces
Vector space
Linear subspace
Linear operator
Function space
Fredholm alternative
Notes and references
Bibliography
External links
Khan Academy, Introduction to the Null Space of a Matrix
Linear algebra
Functional analysis
Matrices
Numerical linear algebra