Determinants and Eigenvalues
Also Eigenvalues and Eigenvectors
How the determinant measures volume change and singularity, and how it leads through the characteristic polynomial to eigenvalues and eigenvectors, the directions a matrix only scales.
Concepts#
- Determinantsigned volume factor , test for invertibility start here
- Eigenvaluethe scaling factors , roots of
- Eigenvectorthe directions with , eigenspaces, eigendecomposition
How it fits together#
The chain. Each concept is built on the previous one:
In practice: compute with the determinant, find its roots (the eigenvalues), then solve the homogeneous system for each root (the eigenspace). That is MML Example 4.5.
One picture behind all three. A linear map in turns the unit square into a parallelogram:
- is its area, and says whether it is mirrored.
- Eigenvectors are the directions that stay on their own line, and eigenvalues the stretch factors along them.
- If the eigenvectors form a basis, the parallelogram spanned by them is mapped to one with sides scaled by . So .
Singularity tests. For these are all the same statement (Invertible Matrix > Properties, Rank and Invertibility):
| Test | Geometric reading |
|---|---|
| volume collapses to | |
| is an eigenvalue | some direction is mapped to |
| there is an eigenvector for | |
| the image is a proper subspace |
Invariants of a linear map. , and the eigenvalues don’t depend on the basis: similar matrices share them. The eigenvectors do change with the basis, as vectors , but they represent the same directions of the map.
How many eigenvectors? The algebraic multiplicity (from ) is an upper bound for the geometric multiplicity ().
| Case | Eigenvectors | Decomposition |
|---|---|---|
| distinct real eigenvalues | basis (Thm. 4.12) | |
| symmetric | orthonormal basis, real (spectral theorem) | |
| repeated eigenvalue, geometric < algebraic multiplicity | too few (defective) | not diagonalizable |
| complex eigenvalues (e.g. rotation) | no real eigenvectors for them | not over |
Symmetric matrices in MSI. The symmetric case is the one that matters for least squares and covariances. A symmetric matrix is positive (semi)definite iff all its eigenvalues are (). By , a positive definite matrix has and is invertible. The converse fails: has .
Key Formulas#
- (Determinant)
- , , , (Determinant)
- , (Eigenvalue, Eigenvector)
- , eigenvalues = roots of (Eigenvalue > Characteristic polynomial)
- , (Eigenvalue > Determinant, trace and invariance)
- (Eigenvector)
- iff the eigenvectors form a basis; for symmetric (Eigenvector > Properties)
Lectures#
- No lecture yet. Source: MML ch. 4.1–4.2, pp. 99–114, eigendecomposition ch. 4.4, pp. 115–117.
Related Topics#
- Rank and Invertibility: rank as the cause of invertibility; and eigenvalues give equivalent tests for square matrices