The Characteristic Equation
How do we find eigenvalues without spinning a vector around by hand? Rewrite
A\vec{v} = \lambda\vec{v} as
(A - \lambda I)\vec{v} = \vec{0}. For a non-zero
\vec{v} to satisfy this, the matrix
A - \lambda I must
collapse
space — its determinant
must be zero:
\det(A - \lambda I) = 0.
This is the characteristic equation. For a 2×2 matrix it expands into a neat
quadratic in \lambda — using the
trace T = a + d and the determinant
D = ad - bc:
\lambda^2 - T\lambda + D = 0.
Roots are eigenvalues
Plotted against \lambda, the characteristic polynomial is a parabola,
and the eigenvalues are exactly where it crosses zero. Slide the trace and
determinant and watch the roots move. Push the curve until it just kisses the axis (a repeated
root) or lifts off it entirely (complex eigenvalues — the matrix is a pure rotation).
A handy shortcut
The quadratic hands you two tidy facts for free: the eigenvalues add up to the
trace (\lambda_1 + \lambda_2 = T) and
multiply to the determinant
(\lambda_1\lambda_2 = D). So a quick glance at a 2×2 matrix often
gives its eigenvalues by inspection. With the eigenvalues in hand, the
eigenvectors
come next.