generalized eigenvector
Let V be a vector space over a field k and T a linear transformation on V (a linear operator). A non-zero vector v∈V is said to be a generalized eigenvector
of T (corresponding to λ) if there is a λ∈k and a positive integer m such that
(T-λI)m(v)=0, |
where I is the identity operator.
In the equation above, it is easy to see that λ is an eigenvalue of T. Suppose that m is the least such integer satisfying the above equation. If m=1, then λ is an eigenvalue of T. If m>1, let w=(T-λI)m-1(v). Then w≠0 (since v≠0) and (T-λI)(w)=0, so λ is again an eigenvalue of T.
Let v be a generalized eigenvector of T corresponding to the eigenvalue λ. We can form a sequence
v,(T-λI)(v),(T-λI)2(v),…,(T-λI)i(v),…,(T-λI)m(v)=0,0,… |
The set Cλ(v) of all non-zero terms in the sequence is called a cycle of generalized eigenvectors of T corresponding to λ. The cardinality m of Cλ(v) is its . For any Cλ(v), write vλ=(T-λI)m-1(v).
Below are some properties of Cλ(v):
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•
vλ is the only eigenvector
of λ in Cλ(v), for otherwise vλ=0.
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•
Cλ(v) is linearly independent
.
Proof.
Let vi=(T-λI)i-1(v), where i=1,…,m. Let 0=∑mi=1rivi with ri∈k. Induct on i. If i=1, then v1=v≠0, so r1=0 and {v1} is linearly independent. Suppose the property is true when i=m-1. Apply T-λI to the equation, and we have 0=∑mi=1ri(T-λI)(vi)=∑m-1i=1rivi+1. Then r1=⋯=rm-1=0 by induction
. So 0=rmvm=rmvλ and thus rm=0 since vλ is an eigenvector and is non-zero. ∎
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More generally, it can be shown that Cλ(v1)∪⋯∪Cλ(vk) is linearly independent whenever {v1λ,…,vkλ} is.
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Let E=span(Cλ(v)). Then E is a (m+1)-dimensional subspace
of the generalized eigenspace
of T corresponding to λ. Furthermore, let T|E be the restriction
of T to E, then [T|E]Cλ(v) is a Jordan block
, when Cλ(v) is ordered (as an ordered basis) by setting
(T-λI)i(v)<(T-λI)j(v) Indeed, for if we let for , then
so that is the matrix given by
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A cycle of generalized eigenvectors is called maximal if . If is finite dimensional, any cycle of generalized eigenvectors can always be extended to a maximal cycle of generalized eigenvectors , meaning that .
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In particular, any eigenvector of can be extended to a maximal cycle of generalized eigenvectors. Any two maximal cycles of generalized eigenvectors extending span the same subspace of .
References
- 1 Friedberg, Insell, Spence. Linear Algebra. Prentice-Hall Inc., 1997.
Title | generalized eigenvector |
---|---|
Canonical name | GeneralizedEigenvector |
Date of creation | 2013-03-22 17:23:13 |
Last modified on | 2013-03-22 17:23:13 |
Owner | CWoo (3771) |
Last modified by | CWoo (3771) |
Numerical id | 13 |
Author | CWoo (3771) |
Entry type | Definition |
Classification | msc 65F15 |
Classification | msc 65-00 |
Classification | msc 15A18 |
Classification | msc 15-00 |
Related topic | GeneralizedEigenspace |
Defines | cycle of generalized eigenvectors |