# Applied linear operators and spectral methods/Lecture 4

## More on spectral decompositions

editIn the course of the previous lecture we essentially proved the following theorem:

### Theorem:

edit1) If a matrix has linearly independent real or complex eigenvectors, the can be diagonalized. 2) If is a matrix whose columns are eigenvectors then is the diagonal matrix of eigenvalues.

The factorization is called the ** spectral representation**
of .

### Application

editWe can use the spectral representation to solve a system of linear homogeneous ordinary differential equations.

For example, we could wish to solve the system

(More generally could be a matrix.)

#### Comment:

editHigher order ordinary differential equations can be reduced to this form. For example,

Introduce

Then the system of equations is

or,

Returning to the original problem, let us find the eigenvalues and eigenvectors of . The characteristic equation is

o we can calculate the eigenvalues as

The eigenvectors are given by

or,

Possible choices of and are

The matrix is one whose columd are the eigenvectors of , i.e.,

and

If the system of equations becomes

Expanded out

The solutions of these equations are

Therefore,

This is the solution of the system of ODEs that we seek.

Most "generic" matrices have linearly independent eigenvectors. Generally a matrix will have distinct eigenvalues unless there are symmetries that lead to repeated values.

### Theorem

editIf has distinct eigenvalues then it has linearly independent eigenvectors.

** Proof:**

We prove this by induction.

Let be the eigenvector corresponding to the eigenvalue . Suppose are linearly independent (note that this is true for = 2). The question then becomes: Do there exist not all zero such that the linear combination

Let us multiply the above by . Then, since , we have

Since is arbitrary, the above is true only when

In thast case we must have

This leads to a contradiction.

Therefore are linearly independent.

Another important class of matrices which are diagonalizable are those which are self-adjoint.

### Theorem

editIf is self-adjoint the following statements are true

- is real for all .
- All eigenvalues are real.
- Eigenvectors of distinct eigenvalues are orthogonal.
- There is an orthonormal basis formed by the eigenvectors.
- The matrix can be diagonalized (this is a consequence of the previous statement.)

** Proof**

1) Because the matrix is self-adjoint we have

From the property of the inner product we have

Therefore,

which implies that is real.

2) Since is real, is real. Also, from the eiegnevalue problem, we have

Therefore, is real.

3) If and are two eigenpairs then

Since the matrix is self-adjoint, we have

Therefore, if , we must have

Hence the eigenvectors are orthogonal.

4) This part is a bit more involved. We need to define a manifold first.

#### Linear manifold

editA linear manifold (or vector subspace) is a subset of which is closed under scalar multiplication and vector addition.

Examples are a line through the origin of -dimensional space, a plane through the origin, the whole space, the zero vector, etc.

#### Invariant manifold

editAn invariant manifold for the matrix is the linear manifold for which implies .

Examples are the null space and range of a matrix . For the case of a rotation about an axis through the origin in -space, invaraiant manifolds are the origin, the plane perpendicular to the axis, the whole space, and the axis itself.

Therefore, if are a basis for and are a basis for (the perpendicular component of ) then in this basis has the representation

We need a matrix of this form for it to be in an invariant manifold for .

Note that if is an invariant manifold of it does not follow that is also an invariant manifold.

Now, if is self adjoint then the entries in the off-diagonal spots must be zero too. In that case, is block diagonal in this basis.

Getting back to part (4), we know that there exists at least one eigenpair ( ) (this is true for any matrix). We now use induction. Suppose that we have found ( ) mutually orthogonal eigenvectors with and are real, . Note that the s are invariant manifolds of as is the space spanned by the s and so is the manifold perpendicular to these vectors).

We form the linear manifold

This is the orthogonal component of the eigenvectors If then

Therefore which means that is invariant.

Hence contains at least one eigenvector with real eigenvalue . We can repeat the procedure to get a diagonal matrix in the lower block of the block diagonal representation of . We then get distinct eigenvectors and so can be diagonalized. This implies that the eigenvectors form an orthonormal basis.

5) This follows from the previous result because each eigenvector can be normalized so that .

We will explore some more of these ideas in the next lecture.

Resource type: this resource contains a lecture or lecture notes. |