Write the operator in divergence form:
The Legendre differential equation therefore gives
These are the eigenvalues of . With the common positive-sign convention for a Sturm-Liouville problem, use instead:
This is a singular Sturm-Liouville problem, because vanishes at the endpoints. Bounded eigenfunctions select the nonlogarithmic branches and satisfy there. The Lagrange identity for a Sturm-Liouville operator gives
The eigenvalues are distinct, proving the orthogonality condition
The weight is one. No choice of normalization of the Legendre polynomials is needed for this conclusion.

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