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1: 25.10 Zeros
More than 41% of all the zeros in the critical strip lie on the critical line (Bui et al. (2011)). …
2: Bibliography B
  • P. Boalch (2005) From Klein to Painlevé via Fourier, Laplace and Jimbo. Proc. London Math. Soc. (3) 90 (1), pp. 167–208.
  • H. M. Bui, B. Conrey, and M. P. Young (2011) More than 41% of the zeros of the zeta function are on the critical line. Acta Arith. 150 (1), pp. 35–64.
  • R. Bulirsch (1965b) Numerical calculation of elliptic integrals and elliptic functions. Numer. Math. 7 (1), pp. 78–90.
  • 3: 19.37 Tables
    Tabulated for ϕ = 0 ( 5 ) 90 , k 2 = 0 ( .01 ) 1 to 10D by Fettis and Caslin (1964). Tabulated for ϕ = 0 ( 1 ) 90 , k 2 = 0 ( .01 ) 1 to 7S by Beli͡akov et al. (1962). … Tabulated for ϕ = 0 ( 5 ) 90 , k = 0 ( .01 ) 1 to 10D by Fettis and Caslin (1964). Tabulated for ϕ = 0 ( 5 ) 90 , arcsin k = 0 ( 1 ) 90 to 6D by Byrd and Friedman (1971), for ϕ = 0 ( 5 ) 90 , arcsin k = 0 ( 2 ) 90 and 5 ( 10 ) 85 to 8D by Abramowitz and Stegun (1964, Chapter 17), and for ϕ = 0 ( 10 ) 90 , arcsin k = 0 ( 5 ) 90 to 9D by Zhang and Jin (1996, pp. 674–675). … Tabulated (with different notation) for ϕ = 0 ( 15 ) 90 , α 2 = 0 ( .1 ) 1 , arcsin k = 0 ( 15 ) 90 to 5D by Abramowitz and Stegun (1964, Chapter 17), and for ϕ = 0 ( 15 ) 90 , α 2 = 0 ( .1 ) 1 , arcsin k = 0 ( 15 ) 90 to 7D by Zhang and Jin (1996, pp. 676–677). …
    4: Errata
  • Subsection 25.10(ii)

    In the paragraph immediately below (25.10.4), it was originally stated that “more than one-third of all zeros in the critical strip lie on the critical line.” which referred to Levinson (1974). This sentence has been updated with “one-third” being replaced with “41%” now referring to Bui et al. (2011) (suggested by Gergő Nemes on 2021-08-23).

  • 5: 20.15 Tables
    This reference gives θ j ( x , q ) , j = 1 , 2 , 3 , 4 , and their logarithmic x -derivatives to 4D for x / π = 0 ( .1 ) 1 , α = 0 ( 9 ) 90 , where α is the modular angle given by … Spenceley and Spenceley (1947) tabulates θ 1 ( x , q ) / θ 2 ( 0 , q ) , θ 2 ( x , q ) / θ 2 ( 0 , q ) , θ 3 ( x , q ) / θ 4 ( 0 , q ) , θ 4 ( x , q ) / θ 4 ( 0 , q ) to 12D for u = 0 ( 1 ) 90 , α = 0 ( 1 ) 89 , where u = 2 x / ( π θ 3 2 ( 0 , q ) ) and α is defined by (20.15.1), together with the corresponding values of θ 2 ( 0 , q ) and θ 4 ( 0 , q ) . Lawden (1989, pp. 270–279) tabulates θ j ( x , q ) , j = 1 , 2 , 3 , 4 , to 5D for x = 0 ( 1 ) 90 , q = 0.1 ( .1 ) 0.9 , and also q to 5D for k 2 = 0 ( .01 ) 1 . Tables of Neville’s theta functions θ s ( x , q ) , θ c ( x , q ) , θ d ( x , q ) , θ n ( x , q ) (see §20.1) and their logarithmic x -derivatives are given in Abramowitz and Stegun (1964, pp. 582–585) to 9D for ε , α = 0 ( 5 ) 90 , where (in radian measure) ε = x / θ 3 2 ( 0 , q ) = π x / ( 2 K ( k ) ) , and α is defined by (20.15.1). …
    6: 5.16 Sums
    For related sums involving finite field analogs of the gamma and beta functions (Gauss and Jacobi sums) see Andrews et al. (1999, Chapter 1) and Terras (1999, pp. 90, 149).
    7: 14.33 Tables
  • Zhang and Jin (1996, Chapter 4) tabulates 𝖯 n ( x ) for n = 2 ( 1 ) 5 , 10 , x = 0 ( .1 ) 1 , 7D; 𝖯 n ( cos θ ) for n = 1 ( 1 ) 4 , 10 , θ = 0 ( 5 ) 90 , 8D; 𝖰 n ( x ) for n = 0 ( 1 ) 2 , 10 , x = 0 ( .1 ) 0.9 , 8S; 𝖰 n ( cos θ ) for n = 0 ( 1 ) 3 , 10 , θ = 0 ( 5 ) 90 , 8D; 𝖯 n m ( x ) for m = 1 ( 1 ) 4 , n m = 0 ( 1 ) 2 , n = 10 , x = 0 , 0.5 , 8S; 𝖰 n m ( x ) for m = 1 ( 1 ) 4 , n = 0 ( 1 ) 2 , 10 , 8S; 𝖯 ν m ( cos θ ) for m = 0 ( 1 ) 3 , ν = 0 ( .25 ) 5 , θ = 0 ( 15 ) 90 , 5D; P n ( x ) for n = 2 ( 1 ) 5 , 10 , x = 1 ( 1 ) 10 , 7S; Q n ( x ) for n = 0 ( 1 ) 2 , 10 , x = 2 ( 1 ) 10 , 8S. Corresponding values of the derivative of each function are also included, as are 6D values of the first 5 ν -zeros of 𝖯 ν m ( cos θ ) and of its derivative for m = 0 ( 1 ) 4 , θ = 10 , 30 , 150 .

  • Belousov (1962) tabulates 𝖯 n m ( cos θ ) (normalized) for m = 0 ( 1 ) 36 , n m = 0 ( 1 ) 56 , θ = 0 ( 2.5 ) 90 , 6D.

  • 8: 33.26 Software
  • Noble (2004). Fortran 90.

  • 9: 4.48 Software
  • Kearfott (1996). Fortran 90.

  • 10: Bibliography S
  • C. W. Schelin (1983) Calculator function approximation. Amer. Math. Monthly 90 (5), pp. 317–325.
  • B. I. Schneider, J. Segura, A. Gil, X. Guan, and K. Bartschat (2010) A new Fortran 90 program to compute regular and irregular associated Legendre functions. Comput. Phys. Comm. 181 (12), pp. 2091–2097.
  • L. Shen (1981) The elliptical microstrip antenna with circular polarization. IEEE Trans. Antennas and Propagation 29 (1), pp. 90–94.
  • R. Sips (1959) Représentation asymptotique des fonctions de Mathieu et des fonctions sphéroidales. II. Trans. Amer. Math. Soc. 90 (2), pp. 340–368.
  • D. M. Smith (2001) Algorithm 814: Fortran 90 software for floating-point multiple precision arithmetic, gamma and related functions. ACM Trans. Math. Software 27 (4), pp. 377–387.