Diagonalisation & powers of a matrix
A is diagonalisable when A = PDP⁻¹ with D diagonal — which happens exactly when there are enough independent eigenvectors to fill the columns of P. The payoff is Aⁿ = PDⁿP⁻¹, and Dⁿ just raises the diagonal entries to the nth power, turning an infeasible computation into a trivial one.
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Method: how to approach it
The order below is what examiners expect to see, and each step carries its own marks.
- Find all eigenvalues and eigenvectorsThe eigenvectors become the columns of P and the corresponding eigenvalues the diagonal of D, IN MATCHING ORDER.
- Check diagonalisabilityYou need n independent eigenvectors. n distinct eigenvalues guarantees this; a repeated eigenvalue needs its eigenspace dimension checked.
- Assemble P and D and invert PVerify with AP = PD, which avoids computing P⁻¹ just to check.
- Compute powersAⁿ = PDⁿP⁻¹, with Dⁿ obtained by raising each diagonal entry to the power n.
Worked example
Diagonalise A = [[2, 1], [0, 3]] and give a formula for Aⁿ.
- A is triangular, so the eigenvalues are the diagonal entries: 2 and 3.
- For λ = 2: (A − 2I) = [[0,1],[0,1]], giving y = 0 and v = (1,0).
- For λ = 3: (A − 3I) = [[−1,1],[0,0]], giving x = y and v = (1,1).
- So P = [[1,1],[0,1]], D = diag(2,3), and P⁻¹ = [[1,−1],[0,1]].
Answer. Aⁿ = P·diag(2ⁿ, 3ⁿ)·P⁻¹ = [[2ⁿ, 3ⁿ − 2ⁿ], [0, 3ⁿ]]. Check n = 1 gives back A ✓.
Where marks get dropped
These are the specific errors that cost credit on diagonalisation & powers of a matrix questions — QED's rubric penalises each of them separately.
- Mismatching the order of eigenvalues in D and eigenvectors in P. Column k of P must correspond to entry k of D.
- Assuming every matrix is diagonalisable. [[1,1],[0,1]] has only one independent eigenvector and is not.
- Computing Aⁿ as PⁿDⁿ(P⁻¹)ⁿ. The intermediate P⁻¹P pairs cancel, which is exactly why Aⁿ = PDⁿP⁻¹ and nothing more.
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Diagonalisation & powers of a matrix — frequently asked questions
When is a matrix guaranteed diagonalisable?
When it has n distinct eigenvalues, or when it is symmetric — the spectral theorem gives real symmetric matrices an orthonormal eigenbasis.
What if it is not diagonalisable?
Use the Jordan normal form, which is block-diagonal with 1s on a superdiagonal. Powers are still computable, just messier.
Why does this matter for recurrences?
A linear recurrence in matrix form has solution vₙ = Aⁿv₀, and diagonalising A gives the closed form — which is precisely how Binet’s Fibonacci formula arises.
The rest of Linear Algebra
Matrices, systems, determinants, eigenvalues. Each subtopic below has its own method, worked example and mark-losing traps.
- 1Matrix arithmetic & inverses
- 2Gaussian elimination
- 3Determinants
- 4Vector spaces, span & linear independence
- 5Basis & dimension
- 6Eigenvalues & eigenvectors
- 7Linear maps & their matrices
- 8Rank, nullity & the rank–nullity theorem
- 9Column space, null space & solution sets
- 10Orthogonality, projections & Gram–Schmidt
- 11Diagonalisation & powers of a matrix
- 12Dot product, norms & angles
- 13Change of basis & similar matrices
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