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11: 23.17 Elementary Properties
λ ( i ) = 1 2 ,
23.17.5 1728 J ( τ ) = q 2 + 744 + 1 96884 q 2 + 214 93760 q 4 + ,
23.17.6 η ( τ ) = n = ( 1 ) n q ( 6 n + 1 ) 2 / 12 .
23.17.8 η ( τ ) = q 1 / 12 n = 1 ( 1 q 2 n ) ,
with q 1 / 12 = e i π τ / 12 .
12: 1.3 Determinants, Linear Operators, and Spectral Expansions
For n = 2 : … for every distinct pair of j , k , or when one of the factors k = 1 n a j k 2 vanishes. … where ω 1 , ω 2 , , ω n are the n th roots of unity (1.11.21). … Let a j , k be defined for all integer values of j and k , and 𝐷 n [ a j , k ] denote the ( 2 n + 1 ) × ( 2 n + 1 ) determinant … Taking l 2 norms, …
13: 24.2 Definitions and Generating Functions
B 2 n + 1 = 0 ,
( 1 ) n + 1 B 2 n > 0 , n = 1 , 2 , .
E 2 n + 1 = 0 ,
( 1 ) n E 2 n > 0 .
24.2.9 E n = 2 n E n ( 1 2 ) = integer ,
14: 26.21 Tables
Andrews (1976) contains tables of the number of unrestricted partitions, partitions into odd parts, partitions into parts ± 2 ( mod 5 ) , partitions into parts ± 1 ( mod 5 ) , and unrestricted plane partitions up to 100. It also contains a table of Gaussian polynomials up to [ 12 6 ] q . …
15: 28.16 Asymptotic Expansions for Large q
Let s = 2 m + 1 , m = 0 , 1 , 2 , , and ν be fixed with m < ν < m + 1 . …
28.16.1 λ ν ( h 2 ) 2 h 2 + 2 s h 1 8 ( s 2 + 1 ) 1 2 7 h ( s 3 + 3 s ) 1 2 12 h 2 ( 5 s 4 + 34 s 2 + 9 ) 1 2 17 h 3 ( 33 s 5 + 410 s 3 + 405 s ) 1 2 20 h 4 ( 63 s 6 + 1260 s 4 + 2943 s 2 + 486 ) 1 2 25 h 5 ( 527 s 7 + 15617 s 5 + 69001 s 3 + 41607 s ) + .
16: 26.10 Integer Partitions: Other Restrictions
The set { 2 , 3 , 4 , } is denoted by T . If more than one restriction applies, then the restrictions are separated by commas, for example, p ( 𝒟 2 , T , n ) . … where the sum is over nonnegative integer values of k for which n 1 2 ( 3 k 2 ± k ) 0 . … where the sum is over nonnegative integer values of k for which n ( 3 k 2 ± k ) 0 . … where the sum is over nonnegative integer values of m for which n 1 2 k m 2 m + 1 2 k m 0 . …
17: 26.2 Basic Definitions
Thus 231 is the permutation σ ( 1 ) = 2 , σ ( 2 ) = 3 , σ ( 3 ) = 1 . … Here σ ( 1 ) = 2 , σ ( 2 ) = 5 , and σ ( 5 ) = 1 . … A lattice path is a directed path on the plane integer lattice { 0 , 1 , 2 , } × { 0 , 1 , 2 , } . … As an example, { 1 , 3 , 4 } , { 2 , 6 } , { 5 } is a partition of { 1 , 2 , 3 , 4 , 5 , 6 } . … As an example, { 1 , 1 , 1 , 2 , 4 , 4 } is a partition of 13. …
18: 5.17 Barnes’ G -Function (Double Gamma Function)
5.17.2 G ( n ) = ( n 2 ) ! ( n 3 ) ! 1 ! , n = 2 , 3 , .
5.17.3 G ( z + 1 ) = ( 2 π ) z / 2 exp ( 1 2 z ( z + 1 ) 1 2 γ z 2 ) k = 1 ( ( 1 + z k ) k exp ( z + z 2 2 k ) ) .
5.17.5 Ln G ( z + 1 ) 1 4 z 2 + z Ln Γ ( z + 1 ) ( 1 2 z ( z + 1 ) + 1 12 ) ln z ln A + k = 1 B 2 k + 2 2 k ( 2 k + 1 ) ( 2 k + 2 ) z 2 k .
Here B 2 k + 2 is the Bernoulli number (§24.2(i)), and A is Glaisher’s constant, given by …
5.17.7 C = lim n ( k = 1 n k ln k ( 1 2 n 2 + 1 2 n + 1 12 ) ln n + 1 4 n 2 ) = γ + ln ( 2 π ) 12 ζ ( 2 ) 2 π 2 = 1 12 ζ ( 1 ) ,
19: Bibliography G
  • W. Gautschi (1973) Algorithm 471: Exponential integrals. Comm. ACM 16 (12), pp. 761–763.
  • É. Goursat (1883) Mémoire sur les fonctions hypergéométriques d’ordre supérieur. Ann. Sci. École Norm. Sup. (2) 12, pp. 261–286, 395–430 (French).
  • V. I. Gromak (1976) The solutions of Painlevé’s fifth equation. Differ. Uravn. 12 (4), pp. 740–742 (Russian).
  • V. I. Gromak (1978) One-parameter systems of solutions of Painlevé equations. Differ. Uravn. 14 (12), pp. 2131–2135 (Russian).
  • J. H. Gunn (1967) Algorithm 300: Coulomb wave functions. Comm. ACM 10 (4), pp. 244–245.
  • 20: 5.23 Approximations
    Cody and Hillstrom (1967) gives minimax rational approximations for ln Γ ( x ) for the ranges 0.5 x 1.5 , 1.5 x 4 , 4 x 12 ; precision is variable. Hart et al. (1968) gives minimax polynomial and rational approximations to Γ ( x ) and ln Γ ( x ) in the intervals 0 x 1 , 8 x 1000 , 12 x 1000 ; precision is variable. … For additional approximations see Hart et al. (1968, Appendix B), Luke (1975, pp. 22–23), and Weniger (2003). … See Luke (1975, pp. 22–23) for additional expansions. …