Is the geometric multiplicity of an eigenvalue a similar invariant?

In summary, the author is saying that if two matrices are diagonalizable, then they are similar. If the matrix is not diagonalizable, it can still be broken down into Jordan normal form. The dimensions of the eigenspaces are invariant under the transformation.
  • #1
Bipolarity
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If two matrices similar to one another are diagonalizable, then certainly this is the case, since the algebraic multiplicity of any eigenvalue they share must be equal (since they are similar), and since they are diagonalizable, those algebraic multiplicities must equal the geometric multiplicities of those eigenvalues. But what if the matrix is not diagonalizable?

BiP
 
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  • #2
The question is equivalent to: if v is an eigenvector of A with eigenvalue [itex] \lambda[/itex], and P is an invertible matrix, find a vector w in terms of v and P such that
[tex] P A P^{-1} w= \lambda w.[/tex]
It's not particularly challenging to construct w
 
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  • #3
matrix not diagonalizable

If the matrix is not diagonalizable then it can still be broken down into Jordan normal form. If an eigenvalue [tex]\lambda[/tex] has multiplicity c, but does not have c independent eigenvectors, you will get Jordan block for each eigenvector.

For example if c = 5 and there are two independent eigenvectors, one with eigenspace of dimension 2 and the other with eigenspace of dimension 3 there will be a Jordan block which is 2x2 and one which is 3x3. The 3x3 Jordan block will look like this:

[tex]
\begin{pmatrix}
\lambda & 1 & 0\\
0 & \lambda & 1\\
0 & 0 & \lambda
\end{pmatrix}
[/tex]

with an nxn block created similarly. All the Jordan blocks reside on the diagonal. If you have reduced two matrices to the same Jordan form, they are, essentially similar.

Re the eigenspaces, the basis of the 2 dimensional one will be the existing eigenvector plus one generalized eigenvector. The 3 dimensional space will also have a basis consisting of the eigenvector plus some combination of generalized eigenvectors.

The dimensions of the eigenspaces are certainly invariant under this transformation.

There is a complete discussion of this in the book Linear Algebra by Peter Lax. Probably other books have it as well. None of them is very clear, but if you spend some time you can figure it out.
 

1. What is the geometric multiplicity of an eigenvalue?

The geometric multiplicity of an eigenvalue is the number of linearly independent eigenvectors associated with that eigenvalue. It represents the number of directions in which a transformation stretches or compresses a vector.

2. Is the geometric multiplicity of an eigenvalue the same as its algebraic multiplicity?

No, the geometric multiplicity and algebraic multiplicity of an eigenvalue are not always the same. The algebraic multiplicity is the number of times an eigenvalue appears as a root of the characteristic polynomial, while the geometric multiplicity is the number of linearly independent eigenvectors associated with that eigenvalue.

3. How is the geometric multiplicity of an eigenvalue related to the dimension of its eigenspace?

The geometric multiplicity of an eigenvalue is equal to the dimension of its associated eigenspace. This means that the number of linearly independent eigenvectors associated with an eigenvalue is equal to the number of basis vectors in its eigenspace.

4. Can the geometric multiplicity of an eigenvalue change?

Yes, the geometric multiplicity of an eigenvalue can change depending on the matrix or linear transformation being considered. If the matrix is diagonalizable, the geometric multiplicity will remain the same. However, for non-diagonalizable matrices, the geometric multiplicity may change for different bases.

5. How is the geometric multiplicity of an eigenvalue important in linear algebra?

The geometric multiplicity of an eigenvalue is important in understanding the behavior of a linear transformation. It provides information about the direction and magnitude of the transformation in a particular direction. Additionally, the geometric multiplicity is used in determining the diagonalizability of a matrix and the existence of a basis of eigenvectors.

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