Let . Differentiating Legendre's differential equation times and using the Leibniz rule gives
The induction step follows by differentiating this equation once: the derivative of the coefficient contributes the additional term . Thus
For fixed , this is negative for every sufficiently large .
Multiplication by puts the equation in self-adjoint form:
Multiply by and integrate over . Regularity and the vanishing factor at both endpoints remove the boundary term in integration by parts, leaving
If is not identically zero, the integral on the right without is positive, whereas the left side is nonnegative. Therefore
Part (a) makes for all sufficiently large , while part (b) would make whenever were nonzero. Hence some derivative of vanishes identically, so is a polynomial.
Let its degree be . Then is a nonzero constant. Substituting into the differentiated equation annihilates both derivative terms and gives
Thus , and
The nonzero regular solutions are therefore constant multiples of the Legendre polynomial of degree .

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