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How is the characteristic equation det(A - λI) = 0 derived from the eigenvector definition Av = λv?

Starting from Av=λvAv = \lambda v, we rewrite the right side as (λI)v(\lambda I)v and move all terms to one side to get (A−λI)v=0(A - \lambda I)v = 0. Since we seek non-zero solutions for vv, the matrix (A−λI)(A - \lambda I) must squash space into a lower dimension (have a non-trivial null space). This occurs if and only if the determinant of (A−λI)(A - \lambda I) is zero.

Conditions

  • vv is a non-zero eigenvector
  • AA is a square matrix
  • II is the identity matrix

Reasoning, step by step

  1. Begin with the definition: Av=λvAv = \lambda v.
  2. Rewrite λv\lambda v as (λI)v(\lambda I)v.
  3. Subtract (λI)v(\lambda I)v from both sides: Av−(λI)v=0Av - (\lambda I)v = 0.
  4. Factor out vv: (A−λI)v=0(A - \lambda I)v = 0.
  5. Argue that for non-zero vv to satisfy this homogeneous system, the matrix (A−λI)(A - \lambda I) must be singular.
  6. Conclude that singularity implies det⁡(A−λI)=0\det(A - \lambda I) = 0.

Example

For the matrix [[3, 1], [0, 2]], setting up (A−λI)(A - \lambda I) gives [[3-λ, 1], [0, 2-λ]]. The determinant is (3−λ)(2−λ)−0=0(3-\lambda)(2-\lambda) - 0 = 0, yielding eigenvalues 3 and 2.

Common misconceptions

  • Assuming det⁡(A)=λdet⁡(I)\det(A) = \lambda \det(I) allows solving directly without forming the shifted matrix.
  • Forgetting that vv must be non-zero, which forces the determinant condition.

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