In mathematics, in linear algebra and functional analysis, a cyclic subspace is a certain special subspace of a vector space associated with a vector in the vector space and a linear transformation of the vector space. The cyclic subspace associated with a vector v in a vector space V and a linear transformation T of V is called the T-cyclic subspace generated by v. The concept of a cyclic subspace is a basic component in the formulation of the cyclic decomposition theorem in linear algebra.
Let
be a linear transformation of a vector space
and let
be a vector in
. The
-cyclic subspace of
generated by
, denoted
, is the subspace of
generated by the set of vectors
. In the case when
is a topological vector space,
is called a cyclic vector for
if
is dense in
. For the particular case of finite-dimensional spaces, this is equivalent to saying that
is the whole space
.
[1]
There is another equivalent definition of cyclic spaces. Let
be a linear transformation of a topological vector space over a field
and
be a vector in
. The set of all vectors of the form
, where
is a polynomial in the ring
of all polynomials in
over
, is the
-cyclic subspace generated by
.[1]
The subspace
is an invariant subspace for
, in the sense that
.
- For any vector space
and any linear operator
on
, the
-cyclic subspace generated by the zero vector is the zero-subspace of
.
- If
is the identity operator then every
-cyclic subspace is one-dimensional.
is one-dimensional if and only if
is a characteristic vector (eigenvector) of
.
- Let
be the two-dimensional vector space and let
be the linear operator on
represented by the matrix
relative to the standard ordered basis of
. Let
. Then
. Therefore
and so
. Thus
is a cyclic vector for
.
Let
be a linear transformation of a
-dimensional vector space
over a field
and
be a cyclic vector for
. Then the vectors
![{\displaystyle B=\{v_{1}=v,v_{2}=Tv,v_{3}=T^{2}v,\ldots v_{n}=T^{n-1}v\}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/69d0d4d13e7aba50b0c54e4f9a75d5d7b21957e4)
form an ordered basis for
. Let the characteristic polynomial for
be
.
Then
![{\displaystyle {\begin{aligned}Tv_{1}&=v_{2}\\Tv_{2}&=v_{3}\\Tv_{3}&=v_{4}\\\vdots &\\Tv_{n-1}&=v_{n}\\Tv_{n}&=-c_{0}v_{1}-c_{1}v_{2}-\cdots c_{n-1}v_{n}\end{aligned}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/8e5c3c585d2cfd118c3c25e54dbdc114298077a6)
Therefore, relative to the ordered basis
, the operator
is represented by the matrix
![{\displaystyle {\begin{bmatrix}0&0&0&\cdots &0&-c_{0}\\1&0&0&\ldots &0&-c_{1}\\0&1&0&\ldots &0&-c_{2}\\\vdots &&&&&\\0&0&0&\ldots &1&-c_{n-1}\end{bmatrix}}}](https://wikimedia.org/api/rest_v1/media/math/render/svg/780b095695dd00bbde9994a70948f7f6a84809bc)
This matrix is called the companion matrix of the polynomial
.[1]