A system of polynomials , , where is of proper degree , is orthonormal on the unit circle with respect to the weight function () if
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where the bar signifies complex conjugate. Simon (2005a, b) gives the general theory of these OP’s in terms of monic OP’s , see §18.33(vi).
Denote
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where , and are constants. Also denote
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where the bar again signifies complex conjugate. Then
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For an alternative and more detailed approach to the recurrence relations, see §18.33(vi).
Assume that . Set
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Let and , , be OP’s with weight functions and , respectively, on . Then
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Conversely,
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where , , , and are independent of .
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with
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For the hypergeometric function see §§15.1 and 15.2(i). Askey (1982a) and Sri Ranga (2010) give more general results leading to what seem to be the right analogues of Jacobi polynomials on the unit circle.
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with
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For the notation, including the basic hypergeometric function , see §§17.2 and 17.4(i).
When the Askey case is also known as the Rogers–Szegő case. See for a more general class Costa et al. (2012).
See Baxter (1961) for general theory. See Askey (1982a) and Pastro (1985) for special cases extending (18.33.13)–(18.33.14) and (18.33.15)–(18.33.16), respectively. See Gasper (1981) and Hendriksen and van Rossum (1986) for relations with Laurent polynomials orthogonal on the unit circle. See Al-Salam and Ismail (1994) for special biorthogonal rational functions on the unit circle.
Instead of orthonormal polynomials Simon (2005a, b) uses monic polynomials . Let be a probability measure on the unit circle of which the support is an infinite set. A system of monic polynomials , , where is of proper degree , is orthogonal on the unit circle with respect to the measure if
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where the bar signifies complex conjugate and , . Then the corresponding orthonormal polynomials are
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If the measure is absolutely continuous, i.e.,
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for some weight function () then (18.33.17) (see also (18.33.1)) takes the form
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For a polynomial
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with complex coefficients and of a certain degree define the reversed polynomial by
| 18.33.22 | |||
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The Verblunsky coefficients (also called Schur parameters or reflection coefficients) are the coefficients in the Szegő recurrence relations
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Then
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Equivalent to the recurrence relations (18.33.23), (18.33.24) are the inverse Szegő recurrence relations
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Combination of (18.33.23) and (18.33.24) gives
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while combination of (18.33.27) and (18.33.23) gives the three-term recurrence relation
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for , while .
For as in (18.33.19) (or more generally as the weight function of the absolutely continuous part of the measure in (18.33.17)) and with the Verblunsky coefficients in (18.33.23), (18.33.24), Szegő’s theorem states that
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By (18.33.25) , so the infinite product in (18.33.31) converges, although the limit may be zero. In particular, by (18.33.31),
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