Academy
Diagonalisation
Level 1 - Math I (Physics) topic page in Linear Maps.
Principle
Diagonalisation rewrites a matrix using a basis of eigenvectors. In that basis, the linear map acts by independent scaling along coordinate directions.
This is powerful in physics because it separates coupled linear behaviour into independent modes.
Notation
Diagonalisation is possible when there are enough linearly independent eigenvectors to form a basis.
Method
Step 1: Find eigenvalues
Solve \(\\det(A-\\lambda I)=0\).
Step 2: Find independent eigenvectors
For each eigenvalue, solve \((A-\\lambda I)\\mathbf v=\\mathbf0\). Collect enough independent eigenvectors to form a basis.
Step 3: Build \(P\) and \(D\)
Put eigenvectors as columns of \(P\). Put the matching eigenvalues in the same order down the diagonal of \(D\).
Rules
If \(A\) has \(n\) distinct eigenvalues, then an \(n\\times n\) matrix is diagonalizable. Repeated eigenvalues require checking whether enough independent eigenvectors exist.
Examples
Checks
- The columns of \(P\) must be independent eigenvectors.
- The order of columns in \(P\) must match the order of eigenvalues in \(D\).
- A matrix with repeated eigenvalues may fail to diagonalise.
- Verify either \(AP=PD\) or \(A=PDP^{-1}\).