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Eigenvalues and diagonalization explain how a square matrix acts along special directions that only get stretched or reversed. This cheat sheet helps students connect computations with the structure of linear transformations. It is useful for solving systems, finding matrix powers, analyzing stability, and understanding change of basis.

Key Facts

  • A scalar λ\lambda is an eigenvalue of AA if there is a nonzero vector v\mathbf{v} such that Av=λvA\mathbf{v} = \lambda \mathbf{v}.
  • The characteristic polynomial of an n×nn \times n matrix AA is p(λ)=det(AλI)p(\lambda) = \det(A - \lambda I) or equivalently det(λIA)\det(\lambda I - A), depending on convention.
  • Eigenvalues are found by solving det(AλI)=0\det(A - \lambda I) = 0.
  • The eigenspace for an eigenvalue λ\lambda is Eλ=Null(AλI)E_{\lambda} = \operatorname{Null}(A - \lambda I).
  • An n×nn \times n matrix AA is diagonalizable if it has nn linearly independent eigenvectors.
  • If A=PDP1A = PDP^{-1}, then the columns of PP are eigenvectors of AA and DD contains the corresponding eigenvalues on its diagonal.
  • If A=PDP1A = PDP^{-1}, then Ak=PDkP1A^k = PD^kP^{-1} for any positive integer kk.
  • The algebraic multiplicity of λ\lambda is its multiplicity as a root of p(λ)p(\lambda), and the geometric multiplicity is dim(Eλ)\dim(E_{\lambda}).

Vocabulary

Eigenvalue
An eigenvalue λ\lambda is a scalar for which Av=λvA\mathbf{v} = \lambda \mathbf{v} has a nonzero solution v\mathbf{v}.
Eigenvector
An eigenvector is a nonzero vector v\mathbf{v} whose direction is unchanged by the transformation AA, so Av=λvA\mathbf{v} = \lambda \mathbf{v}.
Characteristic Polynomial
The characteristic polynomial is p(λ)=det(AλI)p(\lambda) = \det(A - \lambda I) or p(λ)=det(λIA)p(\lambda) = \det(\lambda I - A), and its roots are the eigenvalues.
Eigenspace
The eigenspace EλE_{\lambda} is the set of all vectors satisfying (AλI)v=0(A - \lambda I)\mathbf{v} = \mathbf{0}.
Diagonalizable Matrix
A matrix is diagonalizable if it can be written as A=PDP1A = PDP^{-1} for some invertible matrix PP and diagonal matrix DD.
Geometric Multiplicity
Geometric multiplicity is the number of linearly independent eigenvectors associated with an eigenvalue, equal to dim(Eλ)\dim(E_{\lambda}).

Common Mistakes to Avoid

  • Using the zero vector as an eigenvector is wrong because eigenvectors must be nonzero, even though A0=λ0A\mathbf{0} = \lambda \mathbf{0} is always true.
  • Solving AλI=0A - \lambda I = 0 instead of det(AλI)=0\det(A - \lambda I) = 0 is wrong because eigenvalues come from a determinant equation, not entry-by-entry equality.
  • Assuming repeated eigenvalues always give enough eigenvectors is wrong because algebraic multiplicity can be larger than geometric multiplicity.
  • Mixing the order of eigenvectors in PP and eigenvalues in DD is wrong because each diagonal entry DiiD_{ii} must match the eigenvector in column ii of PP.
  • Trying to diagonalize a matrix without checking independence is wrong because PP is invertible only when its eigenvector columns are linearly independent.

Practice Questions

  1. 1 Find the eigenvalues of A=[2103]A = \begin{bmatrix}2 & 1 \\ 0 & 3\end{bmatrix}.
  2. 2 For A=[4001]A = \begin{bmatrix}4 & 0 \\ 0 & -1\end{bmatrix}, find eigenvectors for each eigenvalue and write a diagonalization A=PDP1A = PDP^{-1}.
  3. 3 Let A=[1101]A = \begin{bmatrix}1 & 1 \\ 0 & 1\end{bmatrix}. Find its eigenvalue and decide whether AA is diagonalizable.
  4. 4 Explain why a matrix with nn distinct eigenvalues must be diagonalizable, but a matrix with repeated eigenvalues might not be.