Multiply the Sturm-Liouville form for by and subtract the equation for multiplied by . Integration givesThe boundary expression is zero because and the functions and first derivatives remain finite. Since are distinct positive integers, this provesFor the derivatives, apply integration by parts once to the same Sturm-Liouville form:Thus the new weight isThis is derivative orthogonality when the Sturm-Liouville potential vanishes. For the derivative is identically zero, which is consistent with the identity.
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