§01What Is an Eigenvector?
Most vectors change direction when multiplied by a matrix. Eigenvectors are the rare exceptions, they only scale.
When you multiply a matrix A by most vectors v, the output Av points in a completely different direction. But certain special vectors satisfy a remarkable property: the matrix only stretches or compresses them, never tilts them.
v is the eigenvector; λ (a scalar) is the eigenvalue.
Geometrically: Av lands on the same line through the origin as v. The eigenvalue λ records the scale factor: λ = 3 triples the vector, λ = −1 flips it, λ = 0 collapses it to zero.
§02Finding Eigenvalues — The Characteristic Polynomial
Rewrite Av = λv as a homogeneous system and demand a non-trivial solution.
Rearranging Av = λv:
For a non-zero solution v to exist, the matrix (A − λI) must be singular:
Expanding det(A − λI) produces a polynomial in λ, the characteristic polynomial p(λ). Its roots are the eigenvalues.
- Form A − λI
Subtract λ from every diagonal entry of A.
- Compute det(A − λI)
Expand to get a polynomial p(λ) of degree n.
- Solve p(λ) = 0
The roots λ₁, λ₂, … are the eigenvalues.
The 2×2 Shortcut
tr(A) = sum of diagonal entries.
§03Finding Eigenvectors — Eigenspaces
Once you know λ, substitute back and solve (A − λI)v = 0.
For each eigenvalue λ, the set of all solutions to (A − λI)v = 0 is the eigenspace E(λ):
Non-zero vectors in E(λ) are the eigenvectors. Note: scalar multiples of eigenvectors are also eigenvectors: they are never unique.
Algebraic vs Geometric Multiplicity
| Multiplicity | Definition | Symbol |
|---|---|---|
| Algebraic (AM) | Power of (λ − λ₀) in p(λ) — how many times λ₀ is a root. | a(λ₀) |
| Geometric (GM) | dim E(λ₀) = dim Null(A − λ₀I). | g(λ₀) |
When GM < AM for any eigenvalue, the matrix is defective (not diagonalisable).
§04Key Properties & Special Cases
Trace, Determinant, and Eigenvalues
These are indispensable verification tools: after computing eigenvalues, check that their sum equals the trace and their product equals the determinant.
Special Matrix Types
| Matrix Type | Eigenvalue Guarantee |
|---|---|
| Symmetric (Aᵀ = A) | All eigenvalues real; eigenvectors for distinct values are orthogonal. |
| Upper/Lower Triangular | Eigenvalues are the diagonal entries. |
| Orthogonal (AᵀA = I) | All eigenvalues satisfy |λ| = 1. |
| Positive Definite | All eigenvalues strictly positive. |
| Nilpotent (Aᵏ = 0) | All eigenvalues are 0. |
§05Ten Worked Examples
From simple 2×2 cases to repeated roots and complex eigenvalues, full procedures throughout.
Find the eigenvalues and eigenvectors of A = [[4,1],[2,3]].
Find eigenvalues and eigenvectors of A = [[3,1],[0,3]].
GM = 1 < AM = 2, so the matrix is defective: not diagonalisable. This is a Jordan block.
λ = 3 (AM=2, GM=1) — defectiveFind eigenvectors of A = 5I₂ (2×2 scalar matrix).
Find eigenvalues of the upper triangular matrix A = [[2,5,−3],[0,−1,4],[0,0,7]].
Verification: tr(A) = 2+(−1)+7 = 8; sum of eigenvalues = 2−1+7 = 8 ✓
λ₁ = 2, λ₂ = −1, λ₃ = 7Find eigenvalues of the rotation matrix R = [[0,−1],[1,0]].
Over ℝ there are no eigenvectors, rotation moves every non-zero vector. Over ℂ the eigenvalues form the conjugate pair ±i, reflecting pure 90° rotation.
λ = i and λ = −i (complex conjugate pair)Find all eigenvalues and eigenvectors of A = [[1,2,0],[0,3,0],[2,−4,2]].
A 2×2 matrix has tr(A) = 5 and det(A) = 6. Find the eigenvalues.
If Av = λv, derive the eigenvalues of A², A⁻¹, and Aᵏ.
Let P project onto a 1-dimensional subspace L ⊂ ℝ². Determine its eigenvalues without computing.
Check: det(P) = 1·0 = 0 (P is singular) ✓
λ = 1 (along L) and λ = 0 (perpendicular to L)Find eigenvectors of the symmetric matrix A = [[2,1],[1,2]] and verify orthogonality.
§06Four Common Mistakes
§07Practice Quiz — 10 Questions
Test yourself before moving on to Diagonalisation.