Laguerre differential operator on polynomials Created 2026-09-24 Updated 2026-09-24
On polynomials with weighted inner product
the operator
is self-adjoint because . Its eigenvalues on polynomials of degree at most are ; its eigenvectors are scalar multiples of the Laguerre polynomials.
A linear operator on a real inner-product space is self-adjoint when
for all .
To prove the finite-dimensional spectral theorem, first note that the continuous quadratic function has a maximum on the unit sphere. The Lagrange multiplier equation at a maximizing vector gives , so has a real unit eigenvector. Its orthogonal complement is invariant because
Induction on the dimension supplies an orthonormal eigenbasis of that complement and hence of .
For ,
while symmetry and bilinearity are immediate, so the displayed formula defines an inner product on . Since
integration by parts gives
The boundary term vanishes for polynomials, proving that is self-adjoint.
On the monomial ,
Thus the matrix of in the monomial basis is triangular with diagonal
These are therefore its eigenvalues. For , corresponding eigenvectors are
for eigenvalues , respectively. They are the first Laguerre polynomials up to normalization, as described by the Laguerre differential operator on polynomials.
Write with . Then
Take to be a small positively oriented circle around . For , start at , travel to , and avoid the pole at zero by a fixed upper or lower detour. The endpoint factor vanishes at , and the exponential controls .
The finite contour extracts the residue at zero:
Only powers occur, and the coefficient of is nonzero. Thus this solution is a polynomial of degree and, up to normalization, is the Laguerre polynomial :
This also follows from the recurrence in part (i), because and every later coefficient vanishes.