Differentiate the power series term by term inside its radius of convergence, and reindex the second derivative so that every coefficient multiplies . The differential equation becomesThe uniqueness of power-series coefficients givesThe even coefficients depend only on and the odd coefficients only on . These are the two local solution branches of the Legendre differential equation around its ordinary point .
For an integer , choose the series whose integer parity agrees with and set the other initial coefficient to zero. At , the numerator in the recurrence vanishes, so and every later coefficient in that integer parity vanishes. With a nonzero coefficient of , this gives a polynomial of degree exactly . Normalize it by .
For , the even branch is constant; for , the odd branch is proportional to . For , the recurrence gives , so normalization fixes . HenceThe opposite-parity branch generally does not terminate; polynomial termination does not mean that both independent solutions become polynomials.
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