Diagonalization and Similarity
Rewriting a matrix in an eigenbasis so that acting, powering, and exponentiating become elementwise operations.
Leads to: The spectral theorem (4.6) guarantees orthogonal diagonalization for symmetric matrices; matrix exponentials drive linear ODEs.
Learning Objectives
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- Define similarity and explain which quantities it preserves.
- Diagonalize a matrix with a full set of independent eigenvectors.
- Use diagonalization to compute matrix powers and functions.
- Diagnose when a matrix is not diagonalizable (defective).
Key Vocabulary
- Similar matrices
- \(A\) and \(B=P^{-1}AP\) for invertible \(P\); same map in different bases.
- Diagonalizable
- \(A=PDP^{-1}\) with \(D\) diagonal; the columns of \(P\) are eigenvectors.
- Eigenbasis
- A basis of the space consisting entirely of eigenvectors of \(A\).
- Algebraic multiplicity
- The multiplicity of \(\lambda\) as a root of the characteristic polynomial.
- Geometric multiplicity
- The dimension \(\dim\ker(A-\lambda I)\) of the eigenspace.
- Defective matrix
- One lacking a full eigenbasis (some eigenvalue’s geometric < algebraic multiplicity); not diagonalizable.
Intuition & Motivation
Similarity
Diagonalization
Diagonalization makes functions of a matrix trivial. Since \(A^k=PD^kP^{-1}\) and \(D^k\) just powers the diagonal, and more generally for any analytic \(f\), \(f(A)=P\,f(D)\,P^{-1}\) with \(f(D)\) applying \(f\) entrywise on the diagonal.
When diagonalization fails
If some eigenvalue’s geometric multiplicity is strictly less than its algebraic multiplicity, there are too few eigenvectors to fill a basis and the matrix is defective. The canonical example is \(\begin{bmatrix}1&1\\0&1\end{bmatrix}\): eigenvalue \(1\) has algebraic multiplicity 2 but only a one-dimensional eigenspace. Such matrices still admit the Jordan form, but not diagonalization.
Explore the map: when two eigen-directions exist and are distinct, the action decomposes into two independent stretches - that is exactly diagonalizability. Tune the entries toward a shear and the eigen-directions merge, previewing a defective matrix.
- Assuming every matrix is diagonalizable - defective matrices (repeated eigenvalues, deficient eigenspaces) are not.
- Ordering the columns of \(P\) inconsistently with the diagonal of \(D\); the \(j\)-th column must match \(\lambda_j\).
- Believing similarity preserves the individual entries; it preserves the eigenvalues/trace/det, not the numbers themselves.
- Using \(A^k=PD^kP^{-1}\) but forgetting to invert \(P\) on the right.
- Distinct eigenvalues ⇒ automatically diagonalizable - you need not even check eigenspaces.
- To power or exponentiate a matrix, diagonalize once and act on the diagonal; this is how linear ODE solutions \(e^{At}\) are computed.
- Symmetric matrices (covariances!) are always diagonalizable, and by an orthogonal \(P\) - the spectral theorem in 4.6.
Knowledge Check
Practical Exercise
Let \(A=\begin{bmatrix}3&0\\1&2\end{bmatrix}\). (a) Find eigenvalues and eigenvectors. (b) Write \(A=PDP^{-1}\). (c) Use it to compute \(A^{3}\).
(a) Triangular, so eigenvalues are the diagonal: \(\lambda=3,2\). For \(\lambda=3\): \((A-3I)=\begin{bmatrix}0&0\\1&-1\end{bmatrix}\Rightarrow x=y\), eigenvector \((1,1)\). For \(\lambda=2\): \(\begin{bmatrix}1&0\\1&0\end{bmatrix}\Rightarrow x=0\), eigenvector \((0,1)\).
(b) \(P=\begin{bmatrix}1&0\\1&1\end{bmatrix},\ D=\begin{bmatrix}3&0\\0&2\end{bmatrix},\ P^{-1}=\begin{bmatrix}1&0\\-1&1\end{bmatrix}\).
(c) \(A^3=PD^3P^{-1}\) with \(D^3=\operatorname{diag}(27,8)\): \(A^3=\begin{bmatrix}27&0\\19&8\end{bmatrix}\) (since the (2,1) entry is \(27-8=19\)). Distinct eigenvalues guaranteed diagonalizability.
Lesson Summary
Formula Sheet Additions
Retrieval Practice
Close the lesson and answer from memory before checking. This is deliberate, effortful recall - the single highest-yield study action.
A: Powers and analytic functions become elementwise on the diagonal: A^k=P D^k P^{-1}, f(A)=P f(D) P^{-1}.
A: When it is defective: some eigenvalue's geometric multiplicity is less than its algebraic multiplicity, so there is no full eigenbasis.
Completion Checklist
- I can explain the core ideas in my own words
- I worked the derivations/examples by hand
- I completed the interactive workbench(es)
- I passed the knowledge check
Source References
This lesson synthesizes and paraphrases concepts from the sources below. No copyrighted text, problem sets, or solutions are reproduced. Return to the originals for full depth.
- Linear Algebra Done Right (Sheldon Axler, 4th ed., 2024) current - Ch. 5 - Ch. 5: eigenspaces, diagonalizable operators, and conditions for diagonalization.
- Numerical Linear Algebra (Trefethen & Bau, SIAM, 1997) foundational - Lec. 24 - Lec. 24: eigenvalue decompositions and similarity transforms.