Content-Length: 576110 | pFad | https://dlmf.nist.gov/./.././././../././15.10.E26
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This is the hypergeometric differential equation. It has regular singularities at , with corresponding exponent pairs , , , respectively. When none of the exponent pairs differ by an integer, that is, when none of , , is an integer, we have the following pairs , of fundamental solutions. They are also numerically satisfactory (§2.7(iv)) in the neighborhood of the corresponding singularity.
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(a) If equals , and , then fundamental solutions in the neighborhood of are given by (15.10.2) with the interpretation (15.2.5) for .
(b) If equals , and , then fundamental solutions in the neighborhood of are given by and
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, | |||
or
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, ; , | |||
or
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, ; , . | |||
(c) If the parameter in the differential equation equals , then fundamental solutions in the neighborhood of are given by times those in (a) and (b), with and replaced throughout by and , respectively.
(d) If equals , or , then fundamental solutions in the neighborhood of are given by those in (a), (b), and (c) with replaced by .
(e) Finally, if equals , or , then fundamental solutions in the neighborhood of are given by times those in (a), (b), and (c) with and replaced by and , respectively.
The three pairs of fundamental solutions given by (15.10.2), (15.10.4), and (15.10.6) can be transformed into 18 other solutions by means of (15.8.1), leading to a total of 24 solutions known as Kummer’s solutions.
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The connection formulas for the principal branches of Kummer’s solutions are:
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