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Eigenvalues & Eigenvectors

Short Notes

For a square matrix A, a scalar λ is called an eigenvalue if there exists a non-zero vector v such that Av = λv. The vector v is called the corresponding eigenvector.

  • Characteristic Equation: \(\det(A - \lambda I) = 0\)
  • Eigenspace: The set of all eigenvectors corresponding to an eigenvalue λ, along with the zero vector, forms a subspace.
  • Algebraic Multiplicity: The number of times λ appears as a root of the characteristic equation.
  • Geometric Multiplicity: The dimension of the eigenspace corresponding to λ.
  • Diagonalizability: A matrix is diagonalizable if and only if algebraic multiplicity = geometric multiplicity for all eigenvalues.

Key Theories & Formulas

1. Properties of Eigenvalues

  • Sum of eigenvalues = Trace(A) = \(\sum_{i} a_{ii}\)
  • Product of eigenvalues = det(A)
  • Eigenvalues of \(A^T\) are same as eigenvalues of \(A\)
  • Eigenvalues of \(A^{-1}\) are \(\frac{1}{\lambda}\) (if A is invertible)
  • Eigenvalues of \(A^k\) are \(\lambda^k\)
  • Eigenvalues of \(A + kI\) are \(\lambda + k\)
  • Eigenvalues of \(kA\) are \(k\lambda\)

2. Special Matrices

Matrix Type Eigenvalue Properties
Symmetric (\(A = A^T\)) All eigenvalues are real
Skew-Symmetric (\(A = -A^T\)) All eigenvalues are purely imaginary or zero
Orthogonal (\(A^T A = I\)) All eigenvalues have magnitude 1
Idempotent (\(A^2 = A\)) Eigenvalues are 0 or 1
Nilpotent (\(A^k = 0\)) All eigenvalues are 0
Involutory (\(A^2 = I\)) Eigenvalues are 1 or -1

3. Cayley-Hamilton Theorem

Every square matrix satisfies its own characteristic equation.

  • If characteristic equation is \(\lambda^2 - 5\lambda + 6 = 0\), then \(A^2 - 5A + 6I = 0\)
  • Useful for computing \(A^{-1}\) and higher powers of \(A\)

4. Diagonalization

If \(A\) is diagonalizable: \(A = PDP^{-1}\)

  • \(P\) = matrix of eigenvectors (column-wise)
  • \(D\) = diagonal matrix of eigenvalues
  • \(A^n = PD^nP^{-1}\) (efficient for computing powers)

Example Problems

Problem 1: Find eigenvalues of \(A = \begin{pmatrix} 4 & 2 \\ 1 & 3 \end{pmatrix}\)

  1. Characteristic equation: \(\det(A - \lambda I) = 0\)
  2. \((4-\lambda)(3-\lambda) - 2 = 0\)
  3. \(\lambda^2 - 7\lambda + 10 = 0\)
  4. \((\lambda - 5)(\lambda - 2) = 0\)
  5. Eigenvalues: λ = 5, 2

Verification:

  • Trace = 4 + 3 = 7 = 5 + 2 ✓
  • Det = 12 - 2 = 10 = 5 × 2 ✓

Problem 2: Find \(A^{100}\) if eigenvalues of \(A\) are 1 and -1.

Using diagonalization: Eigenvalues of \(A^{100}\) are \(1^{100} = 1\) and \((-1)^{100} = 1\).


Hardest GATE Questions

Topic: Cayley-Hamilton & Matrix Powers

Question (GATE 2017 Style): Let \(A\) be a 3×3 matrix with eigenvalues 1, 2, 3. Find the value of \(\det(A^2 - 4A + 3I)\).

Solution:

  1. The eigenvalues of \(A^2 - 4A + 3I\) are obtained by substituting eigenvalues of \(A\) into \(f(\lambda) = \lambda^2 - 4\lambda + 3\)
  2. For \(\lambda_1 = 1\): \(f(1) = 1 - 4 + 3 = 0\)
  3. For \(\lambda_2 = 2\): \(f(2) = 4 - 8 + 3 = -1\)
  4. For \(\lambda_3 = 3\): \(f(3) = 9 - 12 + 3 = 0\)
  5. Eigenvalues of \((A^2 - 4A + 3I)\) are: 0, -1, 0
  6. \(\det(A^2 - 4A + 3I) = 0 \times (-1) \times 0 = \mathbf{0}\)

Why it's hard: Requires understanding that polynomial functions of matrices preserve eigenvalue relationships.


Topic: Geometric vs Algebraic Multiplicity

Question (GATE 2015 Variant): For which value of \(k\) is the matrix \(A = \begin{pmatrix} 2 & 1 & 0 \\ 0 & 2 & k \\ 0 & 0 & 2 \end{pmatrix}\) diagonalizable?

Solution:

  1. Eigenvalue: λ = 2 with algebraic multiplicity 3
  2. For diagonalizability: geometric multiplicity must also be 3
  3. Find eigenspace: \((A - 2I)v = 0\)
  4. \(A - 2I = \begin{pmatrix} 0 & 1 & 0 \\ 0 & 0 & k \\ 0 & 0 & 0 \end{pmatrix}\)
  5. For k ≠ 0: rank = 2, nullity = 1 (not diagonalizable)
  6. For k = 0: rank = 1, nullity = 2 (still not 3)
  7. Never diagonalizable for any k (upper triangular with repeated eigenvalues and non-zero superdiagonal)

References