The Laguerre differential equation is given by
(1)
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Equation (1) is a special case of the more general associated Laguerre differential equation, defined by
(2)
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where and are real numbers (Iyanaga and Kawada 1980, p. 1481; Zwillinger 1997, p. 124) with .
The general solution to the associated equation (2) is
(3)
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where is a confluent hypergeometric function of the first kind and is a generalized Laguerre polynomial.
Note that in the special case , the associated Laguerre differential equation is of the form
(4)
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so the solution can be found using an integrating factor
(5)
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(6)
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(7)
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(8)
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as
(9)
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(10)
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(11)
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where is the En-function.
The associated Laguerre differential equation has a regular singular point at 0 and an irregular singularity at . It can be solved using a series expansion,
(12)
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(13)
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(14)
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(15)
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(16)
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This requires
(17)
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(18)
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for . Therefore,
(19)
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for , 2, ..., so
(20)
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(21)
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(22)
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If is a nonnegative integer, then the series terminates and the solution is given by
(23)
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where is an associated Laguerre polynomial and is a Pochhammer symbol. In the special case , the associated Laguerre polynomial collapses to a usual Laguerre polynomial and the solution collapses to
(24)
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