The -hypergeometric OPβs comprise the -Hahn class (or -linear lattice class) OPβs and the AskeyβWilson class (or -quadratic lattice class) OPβs (Β§18.28). Together they form the -Askey scheme. This scheme gives a graphical representation of all families of OPβs belonging to it together with the limit relations between them, see Koekoek et al. (2010, p.Β 414).
For the notation of -hypergeometric functions see Β§Β§17.2 and 17.4(i). Unless said otherwise, we will assume that . For (17.4.1) with , , and we will use the convention that the summation on the right-hand side ends at .
The -Hahn class OPβs comprise systems of OPβs , , or , that are eigenfunctions of a second order -difference operator. Thus
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where , , and are independent of , and where the are the eigenvalues. In the -Hahn class OPβs the role of the operator in the Jacobi, Laguerre, and Hermite cases is played by the -derivative , as defined in (17.2.41). A (nonexhaustive) classification of such systems of OPβs was made by Hahn (1949). There are 18 families of OPβs of -Hahn class. These families depend on further parameters, in addition to . The generic (top level) cases are the -Hahn polynomials and the big -Jacobi polynomials, each of which depends on three further parameters.
All these systems of OPβs have orthogonality properties of the form
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where is given by or . Here are fixed positive real numbers, and and are sequences of successive integers, finite or unbounded in one direction, or unbounded in both directions. If and are both nonempty, then they are both unbounded to the right. In case of unbounded sequences (18.27.2) can be rewritten as a -integral, see Β§17.2(v), and more generally Gasper and Rahman (2004, (1.11.2)). Some of the systems of OPβs that occur in the classification do not have a unique orthogonality property. Thus in addition to a relation of the form (18.27.2), such systems may also satisfy orthogonality relations with respect to a continuous weight function on some interval.
Here only a few families are mentioned. They are defined by their -hypergeometric representations, followed by their orthogonality properties. For other formulas, including -difference equations, recurrence relations, duality formulas, special cases, and limit relations, see Koekoek et al. (2010, ChapterΒ 14). See also Gasper and Rahman (2004, pp.Β 195β199, 228β230) and Ismail (2009, ChaptersΒ 13, 18, 21).
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with
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Alternative definitions and notations are
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and
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The orthogonality relations are given by (18.27.2), with
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| , , , | |||
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and
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with
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Bounds for the extreme zeros are given in Driver and Jordaan (2013).
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Little -Jacobi polynomials for are called little -Laguerre or Wall polynomials:
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The measure is not uniquely determined:
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and
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| , , | |||
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with
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Bounds for the extreme zeros are given in Driver and Jordaan (2013).
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(Sometimes in the literature is replaced by .)
The measure is not uniquely determined:
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and
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For discrete -HermiteΒ II polynomials the measure is not uniquely determined.
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