power series in q

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1: 28.15 Expansions for Small q
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§28.15(i) Eigenvalues λ ν ⁡ ( q )
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§28.15(ii) Solutions me ν ⁡ ( z , q )
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2: 28.6 Expansions for Small q
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§28.6(i) Eigenvalues
… ►The coefficients of the power series of a 2 ⁢ n ⁡ ( q ) , b 2 ⁢ n ⁡ ( q ) and also a 2 ⁢ n + 1 ⁡ ( q ) , b 2 ⁢ n + 1 ⁡ ( q ) are the same until the terms in q 2 ⁢ n − 2 and q 2 ⁢ n , respectively. … ►
28.6.19 a − ( 2 ⁢ n + 2 ) 2 − q 2 a − ( 2 ⁢ n ) 2 − q 2 a − ( 2 ⁢ n − 2 ) 2 − ⁢ ⋯ ⁢ q 2 a − 2 2 = − q 2 ( 2 ⁢ n + 4 ) 2 − a − q 2 ( 2 ⁢ n + 6 ) 2 − a − ⋯ , a = b 2 ⁢ n + 2 ⁡ ( q ) .
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§28.6(ii) Functions ce n and se n
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3: 28.2 Definitions and Basic Properties
… ►Near q = 0 , a n ⁡ ( q ) and b n ⁡ ( q ) can be expanded in power series in q (see §28.6(i)); elsewhere they are determined by analytic continuation (see §28.7). …
4: 28.34 Methods of Computation
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  • (a)

    Summation of the power series in §§28.6(i) and 28.15(i) when | q | is small.

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  • (a)

    Summation of the power series in §§28.6(ii) and 28.15(ii) when | q | is small.

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    5: 23.17 Elementary Properties
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    §23.17(ii) Power and Laurent Series
    ►When | q | < 1 ►
    23.17.4 λ ⁡ ( τ ) = 16 ⁢ q ⁢ ( 1 − 8 ⁢ q + 44 ⁢ q 2 + ⋯ ) ,
    … ►In (23.17.5) for terms up to q 48 see Zuckerman (1939), and for terms up to q 100 see van Wijngaarden (1953). … ►with q 1 / 12 = e i ⁢ π ⁢ τ / 12 .
    6: 20.11 Generalizations and Analogs
    … ►In the case z = 0 identities for theta functions become identities in the complex variable q , with | q | < 1 , that involve rational functions, power series, and continued fractions; see Adiga et al. (1985), McKean and Moll (1999, pp. 156–158), and Andrews et al. (1988, §10.7). …
    7: 17.18 Methods of Computation
    §17.18 Methods of Computation
    … ►The two main methods for computing basic hypergeometric functions are: (1) numerical summation of the defining series given in §§17.4(i) and 17.4(ii); (2) modular transformations. Method (1) is applicable within the circles of convergence of the defining series, although it is often cumbersome owing to slowness of convergence and/or severe cancellation. Method (2) is very powerful when applicable (Andrews (1976, Chapter 5)); however, it is applicable only rarely. … ►Shanks (1955) applies such methods in several q -series problems; see Andrews et al. (1986).
    8: 16.5 Integral Representations and Integrals
    … ►In this event, the formal power-series expansion of the left-hand side (obtained from (16.2.1)) is the asymptotic expansion of the right-hand side as z → 0 in the sector | ph ⁡ ( − z ) | ≤ ( p + 1 − q − δ ) ⁢ π / 2 , where δ is an arbitrary small positive constant. …
    9: 16.8 Differential Equations
    … ►For other values of the b j , series solutions in powers of z (possibly involving also ln ⁡ z ) can be constructed via a limiting process; compare §2.7(i) in the case of second-order differential equations. … ►In this reference it is also explained that in general when q > 1 no simple representations in terms of generalized hypergeometric functions are available for the fundamental solutions near z = 1 . Analytical continuation formulas for F q q + 1 ⁡ ( 𝐚 ; 𝐛 ; z ) near z = 1 are given in Bühring (1987b) for the case q = 2 , and in Bühring (1992) for the general case. … ►If p ≤ q , then …Thus in the case p = q the regular singularities of the function on the left-hand side at α and ∞ coalesce into an irregular singularity at ∞ . …
    10: 3.10 Continued Fractions
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    §3.10(ii) Relations to Power Series
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    Stieltjes Fractions
    … ►We say that it corresponds to the formal power series … ►For several special functions the S -fractions are known explicitly, but in any case the coefficients a n can always be calculated from the power-series coefficients by means of the quotient-difference algorithm; see Table 3.10.1. … ►We say that it is associated with the formal power series f ⁢ ( z ) in (3.10.7) if the expansion of its n th convergent C n in ascending powers of z , agrees with (3.10.7) up to and including the term in z 2 ⁢ n − 1 , n = 1 , 2 , 3 , … . …