For a positive eigenvalue write . The general solution of the limiting constant-coefficient differential equation is . The endpoint at zero gives . A nonzero eigenfunction then requires , and the endpoint at gives . Consequently
For real eigenfunctions the constants may be any nonzero real amplitudes. Requiring unit L2 norm would set , but that normalization is not required by the question. The lowest eigenvalue is and its eigenspace is spanned by . For completeness, zero yields only an affine solution annihilated by both endpoints, and negative eigenvalues yield hyperbolic functions whose two zero endpoint values also force the zero solution.
The product rule gives and . On an interval avoiding , substitution and division by give
For a constant-coefficient differential equation, the coefficient of forces . At , the remaining coefficient also vanishes. Thus
The characteristic equation of a constant-coefficient differential equation is , with complex conjugate roots of a polynomial . Its real solutions and are linearly independent. Therefore the general solution is
The constants can be chosen independently on the two sides of the singular point. The power substitution reducing a differential equation to constant coefficients here is invertible wherever .
On an interval where the substitution is real and , a factor formed by exponentiation can remove inverse powers from the coefficients of a linear ordinary differential equation. For
the substitution gives
It becomes a constant-coefficient differential equation exactly when , and . Derive this by the product rule; checking only the coefficient of is insufficient.