A Further Result on the Cyclic Subspace ()

Huailei Wang

State Key Laboratory of Mechanics and Control for Mechanical Structures, Nanjing University of Aeronautics and Astronautics, Nanjing, China.

**DOI: **10.4236/alamt.2014.42007
PDF
HTML
3,730
Downloads
5,910
Views
Citations

State Key Laboratory of Mechanics and Control for Mechanical Structures, Nanjing University of Aeronautics and Astronautics, Nanjing, China.

Based on the geometric theories of vector space, a Cross-Identity theorem is proved for the relationship between the power kernels and power images of linear map on its cyclic subspace. By this result, a new approach of proof is found for the fact that a square matrix with only one eigenvalue and one-dimensional eigenspace is similar to a Jordan block matrix.

Keywords

Power Kernel, Power Image, Cyclic Subspace, Jordan Block Matrix, Linear Map

Share and Cite:

Wang, H. (2014) A Further Result on the Cyclic Subspace. *Advances in Linear Algebra & Matrix Theory*, **4**, 96-99. doi: 10.4236/alamt.2014.42007.

1. Introduction

Linear algebra has a wide range of application in most scientific and technological areas. As a fundamental part, the theory of vector space and linear map has developed to be a nearly perfect subject since nineteenth century. In the viewpoint of the author, when applying the theory to diverse problems, the more the detailed aspects of the knowledge one is in possession of, the more proficient one will become in dealing with those related problems. For example, in one of the excellent dynamical system monographs “Differential equations, Dynamical Systems, and an Introduction to Chaos” [1] , the authors put a separate chapter named “Higher Dimensional Linear Algebra” to help the readers recall some relevant linear algebra knowledge needed for the analysis of differential equations and dynamical systems, despite so many linear algebra monographs available for reference, such as [2] -[8] to name a few. Although it is just a brief review of higher dimensional linear algebra, the authors presented therein a distinct method to prove that a matrix can be transformed by a similarity transformation to a Jordan block matrix when it has only one eigenvalue and one-dimensional eigenspace. The essence of the method resides in a subtle analysis of the dimension of the kernel and the image of the matrix. Motivated by this method, this study is intended to generalize the results to the matrix. For this purpose, it is found that it is necessary to gain a deep insight into some geometric properties of the subspace, which finally leads to a more specific relationship discovered between the power-m kernel and the power-m image of linear map, which is reffered to as the Cross-Identity theorem below. As a corollary of this theorem, we proved the fact that a square matrix with only one eigenvalue and one eigenvector is similar to a Jordan block matrix.

The paper is organized as follows. In Section 2, some basic facts will be recalled as preliminaries for the good understanding of the work. Section 3 presents the main results of this paper with some lemmas preceding the Cross-Identity theorem. Some conclusions are drawn finally in Section 4.

2. Preliminaries

Let be a n-dimensional vector space over the complex numbers, and be the set of all linear maps mapping the vector space into itself, and let and denote the kernel (null space) and the image (range) of a linear map, respectively, then it is well known that if the characteristic polynomial of is factorized as, being its distinct eigenvalues, then the vector space can be decomposed into the direct sum of some subspaces, i.e., where with denoting the identity map. Moreover, it can also be proved by using the primary decomposition that each of the above subspace, and hence the whole vector space, can be further expressed as a direct sum of cyclic subspaces [3] . Because the transformation matrix of a linear map under a cyclic basis takes on a Jordan normal form, the above decomposition theories lead straightforward to a geometric approach of proof for the fact that any square matrix can be brought into Jordan normal form through a similarity transformation with a change-of-basis matrix (another way leading to this result is through the elementary divisor theory [7] ).

From the above viewpoint, the cyclic subspace of a vector space shall be an important concept in the field of linear algebra. For the convenience of reference, some preliminary concepts are presented below, for which one can also refer to [3] .

Definition 2.1 Cyclic vector Let be a complex number, let, , then is called if there exists an integer such that. The smallest positive integer having this property will then be called a period of relative to.

Definition 2.2 Cyclic space The vector space will be called cyclic if there exists some number and an element which is and generate.

Theorem 2.3 if is, with period, then are linearly independent.

Definition 2.4 Cyclic basis if is, with period, then is called a cyclic basis or Jodan basis for the cyclic space it generates.

Definition 2.5 Jordan block matrix A matrix is called a Jordan block matrix if it has the same number on the diagonal, 1 above the diagonal, and 0 everywhere else.

Theorem 2.6 Let be a linear map defined on a -dimensional cyclic space, then the associated matrix with respect to the cyclic basis is equal to a Jordan block matrix.

Hence, it has only one eigenvalue and one-dimensional eigenspace.

Definition 2.7 Fan and Fan basis By a fan of linear map A in vector space , we shall mean a sequence of subspaces such that is contained in for each, such that, and finally such that each is. By a fan basis, we shall mean a basis of such that is a basis for.

3. Cross-Identity Theorem

To state the results of this paper, some more notations need to be introduced. As is known, the customary eigenspace of a linear map associated with eigenvalue is equivalent to, and the corresponding generalized eigenspaces are the union set of. For convenience, we refer to and as power-m kernel and power-m image with respect to linear map , respectively. In this case, the customary eigenspace and the generalized eigenspaces associated with eigenvalue are the power-one kernel and the higher power kernels of linear map.

Since a vector space can be expressed as a direct sum of cyclic subspaces, we only consider one of its subspace, or without loss of generality, suppose entirely is a space hereafter. In this situation, according to Theorem 2.6, has only one eigenvalue and one-dimensional eigensapce. In addition, according to the direct sum decomposition of the vector space, there shall be, which means is nilpotent on cyclic space. In what follows, we will show step by step that in this situation, there is a concise relationship between the corresponding power kernels and power images of linear map. For simplicity, the following abbreviations of notations are introduced:

where means the restricted eigenspace in subspace, and means the restricted image of on. In what follows, the power 1 will be omitted when, i.e., , ,. Then it is easy to verify that, ,. The above analysis also readily yields that,.

Now, it is ready to present some further results for a cyclic space as follows.

Lemma 3.1 If, then,.

Proof Note that, are all subspaces, then since, must have an eigenvector in, which implies,. Recall that and, it leads straightforward to. Note, then we have.

Lemma 3.2 If, then,.

Proof implies, then from Lemma 3.1 there will be,. Let, then it follows

which results in, i.e..

From Lemma 3.2, one can see that for a cyclic subspace, the sequence of the dimensions of power images decrease with step one, and hence, the sequence of dimensions of power kernels will increase with step one.

Corollary 3.3.

Proof Note that, there must be. By Lemma 3.2, it follows that. Since, then we have.

Theorem 3.4 (Cross-Identity Theorem) The power kernels and power images of linear map on a cyclic space have the following Cross-Identity relationship, i.e.

Proof By Corollary 3.3, we can know readily that,. Moreover, according to the definition of, , it is easy to verify the following inclusion sequence.

We give the proof in what follows by two steps. The first step is to prove. Since, so for, there is a such that, which yields. Hence, , and therefore. Because and have the same dimension, there must be. Then we have. Next step is to prove,. For, we have. Since, then. Hence, there must exist an such that with. Since, then, which means there must exit an such that with. Carrying on with this procedure, one can find an such that with . Now it can be deduced from above that, i.e., which implies. According to Corollary 3.3, , thus, we can readily contend that.

Corollary 3.5 Suppose matrix has only one eigenvalue, and the corresponding eigenspace v is one dimensional, then there must exist a transformation matrix such that is a Jordan block matrix.

Proof Let matrix be the associated matrix of a linear map under a basis. Since, then there must be an such that, i.e.. Let, then it is easy to verify that constitutes a fan basis of. Thus, it is available to define an invertible linear transformation with an invertible transformation matrix T, such that

Notice that, we have, i.e.. Then,. From the above transformation we can contend that is a Jordan block matrix with the following form

4. Conclusion

This paper studies some special properties of cyclic subspaces. Although it is well known that the dimensions of the power kernels of a linear map on a vector space are decreasing, and the corresponding power images are increasing, i.e. and, we show in this paper that for a cyclic subspace, the sequence of the dimensions of power kernels increases with step one, and the sequence of dimensions of power images decreases with step one. Besides, we find a Cross-Identity relationship between the power kernels and the power images, which is peculiar to cyclic subspaces. Another contribution of this paper is that we find a new way, by the application of the cross-identity theorem, to prove that a square matrix with only one eigenvalue and one-dimensional eigenspace is similar to a Jordan block matrix.

Acknowledgements

This work is supported by the National Natural Science Foundation of China (Grant No. 11172126). We also would like to thank the referees for their comments and suggestions.

Conflicts of Interest

The authors declare no conflicts of interest.

[1] | Hirsch, M.W., Smale, S. and Devaney R.L. (2004) Differential Equations, Dynamical Systems, and an Introduction to Chaos. 2nd Edition, Elsevier Academic Press, San Diego. |

[2] | Greub, W.H. (1967) Linear Algebra. 3rd Edition, Springer, Berlin. |

[3] | Lancaster, P. and Tismenetsky, M. (1985) The Theory of Matrices: With Applications. Academic Press Inc., San Diego. |

[4] |
Lang, S. (1987) Linear Algebra. 3rd Edition, Springer, New York. http://dx.doi.org/10.1007/978-1-4757-1949-9 |

[5] |
Axler, S. (1997) Linear Algebra Done Right. Springer, New York. http://dx.doi.org/10.1007/b97662 |

[6] | Lax, P.D. (2007) Linear Algebra and Its Applications. 2nd Edition, John Wiley & Sons Inc, Hoboken, New Jersey. |

[7] | Roman, S. (2008) Advanced Linear Algebra. 3rd Edition, Springer, New York. |

[8] | Xu, Y.C. (2008) Linear Algebra and Matrix Theory. 2nd Edition, High Education Press, Beijing (in Chinese). |

Journals Menu

Contact us

+1 323-425-8868 | |

customer@scirp.org | |

+86 18163351462(WhatsApp) | |

1655362766 | |

Paper Publishing WeChat |

Copyright © 2024 by authors and Scientific Research Publishing Inc.

This work and the related PDF file are licensed under a Creative Commons Attribution 4.0 International License.