-
(Friedberg 5.10) Let
be a linear operator on and let be distinct eigenvalues of . If are the corresponding eigenvectors then are linearly independent. -
Let
be an eigenvalue of , a linear operator over . The set is called the Eigenspace of
corresponding to eigenvalue . For a matrix
, the eigenspace of is the eigenspace of . The eigenspace is a subspace of
. -
We define the geometric multiplicity as
That is, it is the dimension of the eigenspace
-
(Friedberg 5.12) Let
be a linear operator on a finite dimensional vector space . If is an eigenvalue of , then . - Intuition: The geometric multiplicity is not necessarily the same as the algebraic multiplicity. By definition, an eigenvector must be nonzero. However, the zero vector may appear as a solution to the linear system corresponding to
. Furthermore cannot exceed because that implies there are more than eigenvectors, that appears more than .
- Intuition: The geometric multiplicity is not necessarily the same as the algebraic multiplicity. By definition, an eigenvector must be nonzero. However, the zero vector may appear as a solution to the linear system corresponding to
-
(Friedberg Lem.5.13) Let
be a linear operator on and be distinct eigenvalues of . For each let . If Then
- Proof: The
’s form a linearly independent set. Therefore, the only non-trivial way to get is to set all .
- Proof: The
-
(Friedberg 5.13) Let
be a linear operator on and be distinct eigenvalues of . Let be a finite linearly independent subset of . Then is a linearly independent subset of
-
(Friedberg 5.14) Let
be a linear operator on a finite vector space such that the characteristic polynomial of splits. Let be distinct eigenvalues of . Then is diagonalizable if and only if the for all . - If
is diagonalizable and is a basis for then forms a basis forcalled the eigenbasis. It contains eigenvectors of .
-
(Friedberg 5.16) Let
be a linear operator on a finite dimensional vector space . is diagonalizable if and only if is the direct sum of the eigenspaces of . - Suppose
is diagonalizable. Each eigenspace is -invariant with characteristic polynomial . Which means by (Friedberg 5.29) The characteristic polynomial of is the product Whereis the algebraic multiplicity of each eigenvalue, equal to the dimension of the corresponding eigenspace.
- Suppose
-
If
is a diagonalizable matrix, then it has an eigendecomposition which is obtained using the change of coordinate matrix Where
is the matrix consisting of linearly independent eigenvalues and .
Spectral Theorem
Links
- Friedberg, Insel and Spence - Ch. 5