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The -radii of convergence will depend on , and in first instance we will assume for Jacobi, ultraspherical, Chebyshev and Legendre, for Laguerre, and for Hermite. With the notation of §§10.2(ii), 10.25(ii), 15.2, and 16.2,
18.12.1 | |||
, , | |||
18.12.2 | |||
18.12.2_5 | |||
, , | |||
with arbitrary. Note that (18.12.2_5) yields (18.12.1) by putting and (18.12.2) by replacing by and next letting .
18.12.3 | |||
, | |||
18.12.3_5 | |||
, | |||
and similar formulas as (18.12.3) and (18.12.3_5) by symmetry; compare the second row in Table 18.6.1. See Ismail (2009, (4.3.2)) for another variant of (18.12.3).
18.12.4 | |||
. | |||
18.12.5 | |||
. | |||
18.12.6 | |||
. | |||
18.12.7 | ||||
. | ||||
18.12.8 | ||||
. | ||||
18.12.9 | |||
. | |||
18.12.10 | |||
. | |||
18.12.11 | |||
. | |||
18.12.12 | |||
18.12.13 | |||
. | |||
18.12.14 | |||
18.12.15 | |||
18.12.16 | |||
18.12.17 | |||
. | |||
See §18.18(vii) for Poisson kernels; these are special cases of bilateral generating functions.
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