The Legendre differential equation is the second-order ordinary differential equation
(1)
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which can be rewritten
(2)
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The above form is a special case of the so-called "associated Legendre differential equation" corresponding to the case . The Legendre differential equation has regular singular points at , 1, and .
If the variable is replaced by , then the Legendre differential equation becomes
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derived below for the associated () case.
Since the Legendre differential equation is a second-order ordinary differential equation, it has two linearly independent solutions. A solution which is regular at finite points is called a Legendre function of the first kind, while a solution which is singular at is called a Legendre function of the second kind. If is an integer, the function of the first kind reduces to a polynomial known as the Legendre polynomial.
The Legendre differential equation can be solved using the Frobenius method by making a series expansion with ,
(4)
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(5)
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Plugging in,
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(11)
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(12)
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(13)
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(14)
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so each term must vanish and
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(16)
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Therefore,
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(20)
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(21)
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(22)
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so the even solution is
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Similarly, the odd solution is
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If is an even integer, the series reduces to a polynomial of degree with only even powers of and the series diverges. If is an odd integer, the series reduces to a polynomial of degree with only odd powers of and the series diverges. The general solution for an integer is then given by the Legendre polynomials
(25)
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where is chosen so as to yield the normalization and is a hypergeometric function.
A generalization of the Legendre differential equation is known as the associated Legendre differential equation.
Moon and Spencer (1961, p. 155) call the differential equation
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the Legendre wave function equation (Zwillinger 1997, p. 124).