Multiply the differential equation by . Sincethe Sturm-Liouville form isThe weighted inner product is consequently . These endpoints are singular: vanishes and diverges, though is integrable. The required boundedness of makes the boundary factors vanish, which is the fact needed in the integration identities below.
Use the real eigenfunctions, or insert a complex conjugate on the first factor for complex functions. Multiply by , do the same with interchanged, and subtract. Integration by parts givesThe boundary term vanishes because both functions and derivatives are bounded while . For distinct squared indices, orthogonality of Sturm-Liouville eigenfunctions therefore yieldsA second integration by parts, using the equation for , givesThus derivative orthogonality when the Sturm-Liouville potential vanishes givesThe index qualification matters. The source initially allows integer indices, so alone does not imply distinct eigenvalues: gives the same . Taking the conventional nonnegative labels makes the stated conclusion valid. For the polynomial solutions below, , so opposite indices are an explicit counterexample to an unqualified orthogonality claim.
For nonnegative integer , De Moivre's theorem makes its polynomial nature explicit:Every term is a polynomial of degree at most . For , the coefficient of is , so its polynomial degree is exactly . These are the Chebyshev polynomials . Their polynomial form also proves the required boundedness of the function and derivative at both endpoints. Negative labels reproduce and have degree .
The first three areUnder , their cross inner products become integrals of , and on . The constant-cosine integrals vanish, and also integrates to zero. Thus all three pairs are orthogonal. Their squared weighted norms are , respectively; more generally
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