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1: 34.3 Basic Properties: 3 ⁒ j Symbol
β–ΊThe left- and right-hand sides of (34.3.22) are known, respectively, as Gaunt’s integral and the Gaunt coefficient (Gaunt (1929)).
2: 10.37 Inequalities; Monotonicity
β–ΊSee also Paltsev (1999), Petropoulou (2000), Segura (2011) and Gaunt (2014).
3: Bibliography G
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  • J. A. Gaunt (1929) The triplets of helium. Philos. Trans. Roy. Soc. London Ser. A 228, pp. 151–196.
  • β–Ί
  • R. E. Gaunt (2014) Inequalities for modified Bessel functions and their integrals. J. Math. Anal. Appl. 420 (1), pp. 373–386.
  • β–Ί
  • W. Gautschi (2009) Variable-precision recurrence coefficients for nonstandard orthogonal polynomials. Numer. Algorithms 52 (3), pp. 409–418.
  • β–Ί
  • K. Goldberg, F. T. Leighton, M. Newman, and S. L. Zuckerman (1976) Tables of binomial coefficients and Stirling numbers. J. Res. Nat. Bur. Standards Sect. B 80B (1), pp. 99–171.
  • 4: 26.3 Lattice Paths: Binomial Coefficients
    §26.3 Lattice Paths: Binomial Coefficients
    β–Ί
    §26.3(i) Definitions
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    §26.3(ii) Generating Functions
    β–Ί
    §26.3(iii) Recurrence Relations
    β–Ί
    §26.3(iv) Identities
    5: 26.21 Tables
    §26.21 Tables
    β–ΊAbramowitz and Stegun (1964, Chapter 24) tabulates binomial coefficients ( m n ) for m up to 50 and n up to 25; extends Table 26.4.1 to n = 10 ; tabulates Stirling numbers of the first and second kinds, s ⁑ ( n , k ) and S ⁑ ( n , k ) , for n up to 25 and k up to n ; tabulates partitions p ⁑ ( n ) and partitions into distinct parts p ⁑ ( π’Ÿ , n ) for n up to 500. … β–ΊGoldberg et al. (1976) contains tables of binomial coefficients to n = 100 and Stirling numbers to n = 40 .
    6: 28.14 Fourier Series
    β–ΊThe coefficients satisfy β–Ί
    28.14.4 q ⁒ c 2 ⁒ m + 2 ( a ( ν + 2 ⁒ m ) 2 ) ⁒ c 2 ⁒ m + q ⁒ c 2 ⁒ m 2 = 0 , a = λ ν ⁑ ( q ) , c 2 ⁒ m = c 2 ⁒ m ν ⁑ ( q ) ,
    β–Ί
    28.14.5 m = ( c 2 ⁒ m ν ⁑ ( q ) ) 2 = 1 ;
    β–Ί
    28.14.7 c 2 ⁒ m ν ⁑ ( q ) = c 2 ⁒ m ν ⁑ ( q ) ,
    β–Ί
    28.14.8 c 2 ⁒ m ν ⁑ ( q ) = ( 1 ) m ⁒ c 2 ⁒ m ν ⁑ ( q ) .
    7: 26.4 Lattice Paths: Multinomial Coefficients and Set Partitions
    §26.4 Lattice Paths: Multinomial Coefficients and Set Partitions
    β–Ί
    §26.4(i) Definitions
    β–Ί M 1 is the multinominal coefficient (26.4.2): … β–Ί
    §26.4(ii) Generating Function
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    §26.4(iii) Recurrence Relation
    8: 29.20 Methods of Computation
    β–ΊSubsequently, formulas typified by (29.6.4) can be applied to compute the coefficients of the Fourier expansions of the corresponding Lamé functions by backward recursion followed by application of formulas typified by (29.6.5) and (29.6.6) to achieve normalization; compare §3.6. … β–ΊA third method is to approximate eigenvalues and Fourier coefficients of Lamé functions by eigenvalues and eigenvectors of finite matrices using the methods of §§3.2(vi) and 3.8(iv). …The approximations converge geometrically (§3.8(i)) to the eigenvalues and coefficients of Lamé functions as n . … β–Ί
    §29.20(ii) Lamé Polynomials
    β–ΊThe corresponding eigenvectors yield the coefficients in the finite Fourier series for Lamé polynomials. …
    9: 15.7 Continued Fractions
    β–Ί
    15.7.1 𝐅 ⁑ ( a , b ; c ; z ) 𝐅 ⁑ ( a , b + 1 ; c + 1 ; z ) = t 0 u 1 ⁒ z t 1 u 2 ⁒ z t 2 u 3 ⁒ z t 3 β‹― ,
    β–Ίwhere … β–Ί β–Ίwhere …
    10: 28.4 Fourier Series
    β–Ί
    §28.4(ii) Recurrence Relations
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    §28.4(iii) Normalization
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    §28.4(v) Change of Sign of q
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    §28.4(vi) Behavior for Small q
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    §28.4(vii) Asymptotic Forms for Large m