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11: Bibliography B
  • W. N. Bailey (1928) Products of generalized hypergeometric series. Proc. London Math. Soc. (2) 28 (2), pp. 242–254.
  • W. N. Bailey (1929) Transformations of generalized hypergeometric series. Proc. London Math. Soc. (2) 29 (2), pp. 495–502.
  • G. Baxter (1961) Polynomials defined by a difference system. J. Math. Anal. Appl. 2 (2), pp. 223–263.
  • E. Berti and V. Cardoso (2006) Quasinormal ringing of Kerr black holes: The excitation factors. Phys. Rev. D 74 (104020), pp. 1–27.
  • S. Bochner (1929) Über Sturm-Liouvillesche Polynomsysteme. Math. Z. 29 (1), pp. 730–736.
  • 12: 4.17 Special Values and Limits
    Table 4.17.1: Trigonometric functions: values at multiples of 1 12 π .
    θ sin θ cos θ tan θ csc θ sec θ cot θ
    π / 12 1 4 2 ( 3 1 ) 1 4 2 ( 3 + 1 ) 2 3 2 ( 3 + 1 ) 2 ( 3 1 ) 2 + 3
    π / 4 1 2 2 1 2 2 1 2 2 1
    2 π / 3 1 2 3 1 2 3 2 3 3 2 1 3 3
    3 π / 4 1 2 2 1 2 2 1 2 2 1
    4.17.3 lim z 0 1 cos z z 2 = 1 2 .
    13: 26.4 Lattice Paths: Multinomial Coefficients and Set Partitions
    For k = 2 M 2 is the number of permutations of { 1 , 2 , , n } with a 1 cycles of length 1, a 2 cycles of length 2, , and a n cycles of length n : … M 3 is the number of set partitions of { 1 , 2 , , n } with a 1 subsets of size 1, a 2 subsets of size 2, , and a n subsets of size n : …For each n all possible values of a 1 , a 2 , , a n are covered. … where the summation is over all nonnegative integers n 1 , n 2 , , n k such that n 1 + n 2 + + n k = n . …
    14: 28.15 Expansions for Small q
    28.15.1 λ ν ( q ) = ν 2 + 1 2 ( ν 2 1 ) q 2 + 5 ν 2 + 7 32 ( ν 2 1 ) 3 ( ν 2 4 ) q 4 + 9 ν 4 + 58 ν 2 + 29 64 ( ν 2 1 ) 5 ( ν 2 4 ) ( ν 2 9 ) q 6 + .
    28.15.2 a ν 2 q 2 a ( ν + 2 ) 2 q 2 a ( ν + 4 ) 2 = q 2 a ( ν 2 ) 2 q 2 a ( ν 4 ) 2 .
    28.15.3 me ν ( z , q ) = e i ν z q 4 ( 1 ν + 1 e i ( ν + 2 ) z 1 ν 1 e i ( ν 2 ) z ) + q 2 32 ( 1 ( ν + 1 ) ( ν + 2 ) e i ( ν + 4 ) z + 1 ( ν 1 ) ( ν 2 ) e i ( ν 4 ) z 2 ( ν 2 + 1 ) ( ν 2 1 ) 2 e i ν z ) + ;
    15: Staff
  • Frank W. J. Olver, University of Maryland and NIST, Chaps. 1, 2, 4, 9, 10

  • Hans Volkmer, University of Wisconsin, Milwaukee, Chaps. 29, 30

  • Roderick S. C. Wong, City University of Hong Kong, Chaps. 1, 2, 18

  • Hans Volkmer, University of Wisconsin–Milwaukee, for Chaps. 29, 30

  • Roderick S. C. Wong, City University of Hong Kong, for Chaps. 2, 18

  • 16: Publications
  • D. W. Lozier, B. R. Miller and B. V. Saunders (1999) Design of a Digital Mathematical Library for Science, Technology and Education, Proceedings of the IEEE Forum on Research and Technology Advances in Digital Libraries (IEEE ADL ’99, Baltimore, Maryland, May 19, 1999). PDF
  • Q. Wang and B. V. Saunders (2005) Web-Based 3D Visualization in a Digital Library of Mathematical Functions, Proceedings of the Web3D Symposium, Bangor, UK, March 29–April 1, 2005. PDF
  • B. V. Saunders and Q. Wang (2006) From B-Spline Mesh Generation to Effective Visualizations for the NIST Digital Library of Mathematical Functions, in Curve and Surface Design, Proceedings of the Sixth International Conference on Curves and Surfaces, Avignon, France June 29–July 5, 2006, pp. 235–243. PDF
  • B. I. Schneider, B. R. Miller and B. V. Saunders (2018) NIST’s Digital Library of Mathematial Functions, Physics Today 71, 2, 48 (2018), pp. 48–53. PDF
  • 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: 28.6 Expansions for Small q
    For more details on these expansions and recurrence relations for the coefficients see Frenkel and Portugal (2001, §2). 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. … Here j = 1 for a 2 n ( q ) , j = 2 for b 2 n + 2 ( q ) , and j = 3 for a 2 n + 1 ( q ) and b 2 n + 1 ( q ) . … where k is the unique root of the equation 2 E ( k ) = K ( k ) in the interval ( 0 , 1 ) , and k = 1 k 2 . … For more details on these expansions and recurrence relations for the coefficients see Frenkel and Portugal (2001, §2). …
    19: 6.14 Integrals
    6.14.2 0 e a t Ci ( t ) d t = 1 2 a ln ( 1 + a 2 ) , a > 0 ,
    6.14.4 0 E 1 2 ( t ) d t = 2 ln 2 ,
    6.14.6 0 Ci 2 ( t ) d t = 0 si 2 ( t ) d t = 1 2 π ,
    6.14.7 0 Ci ( t ) si ( t ) d t = ln 2 .
    For collections of integrals, see Apelblat (1983, pp. 110–123), Bierens de Haan (1939, pp. 373–374, 409, 479, 571–572, 637, 664–673, 680–682, 685–697), Erdélyi et al. (1954a, vol. 1, pp. 40–42, 96–98, 177–178, 325), Geller and Ng (1969), Gradshteyn and Ryzhik (2000, §§5.2–5.3 and 6.2–6.27), Marichev (1983, pp. 182–184), Nielsen (1906b), Oberhettinger (1974, pp. 139–141), Oberhettinger (1990, pp. 53–55 and 158–160), Oberhettinger and Badii (1973, pp. 172–179), Prudnikov et al. (1986b, vol. 2, pp. 24–29 and 64–92), Prudnikov et al. (1992a, §§3.4–3.6), Prudnikov et al. (1992b, §§3.4–3.6), and Watrasiewicz (1967).
    20: 25.15 Dirichlet L -functions
    with the product taken over all primes p , beginning with p = 2 . …
    25.15.5 L ( 1 s , χ ) = k s 1 Γ ( s ) ( 2 π ) s ( e π i s / 2 + χ ( 1 ) e π i s / 2 ) G ( χ ) L ( s , χ ¯ ) ,
    25.15.7 L ( 2 n , χ ) = 0  if  χ ( 1 ) = 1 , n = 0 , 1 , 2 , ,
    25.15.8 L ( 2 n 1 , χ ) = 0  if  χ ( 1 ) = 1 , n = 0 , 1 , 2 , .
    There are also infinitely many zeros in the critical strip 0 s 1 , located symmetrically about the critical line s = 1 2 , but not necessarily symmetrically about the real axis. …