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1: 12.11 Zeros
§12.11(iii) Asymptotic Expansions for Large Parameter
12.11.5 p 0 ( ζ ) = t ( ζ ) ,
12.11.6 p 1 ( ζ ) = t 3 6 t 24 ( t 2 1 ) 2 + 5 48 ( ( t 2 1 ) ζ 3 ) 1 2 .
12.11.8 q 0 ( ζ ) = t ( ζ ) .
12.11.9 u a , 1 2 1 2 μ ( 1 1.85575 708 μ 4 / 3 0.34438 34 μ 8 / 3 0.16871 5 μ 4 0.11414 μ 16 / 3 0.0808 μ 20 / 3 ) ,
2: Bibliography D
  • C. de la Vallée Poussin (1896a) Recherches analytiques sur la théorie des nombres premiers. Première partie. La fonction ζ ( s ) de Riemann et les nombres premiers en général, suivi d’un Appendice sur des réflexions applicables à une formule donnée par Riemann. Ann. Soc. Sci. Bruxelles 20, pp. 183–256 (French).
  • C. de la Vallée Poussin (1896b) Recherches analytiques sur la théorie des nombres premiers. Deuxième partie. Les fonctions de Dirichlet et les nombres premiers de la forme linéaire M x + N . Ann. Soc. Sci. Bruxelles 20, pp. 281–397 (French).
  • B. Döring (1966) Complex zeros of cylinder functions. Math. Comp. 20 (94), pp. 215–222.
  • T. M. Dunster (1989) Uniform asymptotic expansions for Whittaker’s confluent hypergeometric functions. SIAM J. Math. Anal. 20 (3), pp. 744–760.
  • T. M. Dunster (1990a) Bessel functions of purely imaginary order, with an application to second-order linear differential equations having a large parameter. SIAM J. Math. Anal. 21 (4), pp. 995–1018.
  • 3: 3.8 Nonlinear Equations
  • (a)

    f ( x 0 ) f ′′ ( x 0 ) > 0 and f ( x ) , f ′′ ( x ) do not change sign between x 0 and ξ (monotonic convergence).

  • (b)

    f ( x 0 ) f ′′ ( x 0 ) < 0 , f ( x ) , f ′′ ( x ) do not change sign in the interval ( x 0 , x 1 ) , and ξ [ x 0 , x 1 ] (monotonic convergence after the first iteration).

  • Then the sensitivity of a simple zero z to changes in α is given by … Consider x = 20 and j = 19 . We have p ( 20 ) = 19 ! and a 19 = 1 + 2 + + 20 = 210 . …
    4: 20.11 Generalizations and Analogs
    20.11.4 f ( a , b ) = θ 3 ( z | τ ) .
    §20.11(iii) Ramanujan’s Change of Base
    These results are called Ramanujan’s changes of base. …
    5: 12.10 Uniform Asymptotic Expansions for Large Parameter
    §12.10 Uniform Asymptotic Expansions for Large Parameter
    §12.10(vi) Modifications of Expansions in Elementary Functions
    Modified Expansions
    6: 20.10 Integrals
    §20.10(i) Mellin Transforms with respect to the Lattice Parameter
    §20.10(ii) Laplace Transforms with respect to the Lattice Parameter
    Then
    20.10.4 0 e s t θ 1 ( β π 2 | i π t 2 ) d t = 0 e s t θ 2 ( ( 1 + β ) π 2 | i π t 2 ) d t = s sinh ( β s ) sech ( s ) ,
    20.10.5 0 e s t θ 3 ( ( 1 + β ) π 2 | i π t 2 ) d t = 0 e s t θ 4 ( β π 2 | i π t 2 ) d t = s cosh ( β s ) csch ( s ) .
    7: 27.2 Functions
    Euclid’s Elements (Euclid (1908, Book IX, Proposition 20)) gives an elegant proof that there are infinitely many primes. …
    27.2.3 π ( x ) x ln x .
    27.2.4 p n n ln n .
    is the sum of the α th powers of the divisors of n , where the exponent α can be real or complex. …
    27.2.14 Λ ( n ) = ln p , n = p a ,
    8: Bibliography K
  • R. B. Kearfott, M. Dawande, K. Du, and C. Hu (1994) Algorithm 737: INTLIB: A portable Fortran 77 interval standard-function library. ACM Trans. Math. Software 20 (4), pp. 447–459.
  • M. K. Kerimov (1980) Methods of computing the Riemann zeta-function and some generalizations of it. USSR Comput. Math. and Math. Phys. 20 (6), pp. 212–230.
  • S. Kida (1981) A vortex filament moving without change of form. J. Fluid Mech. 112, pp. 397–409.
  • A. V. Kitaev and A. H. Vartanian (2004) Connection formulae for asymptotics of solutions of the degenerate third Painlevé equation. I. Inverse Problems 20 (4), pp. 1165–1206.
  • T. H. Koornwinder (2009) The Askey scheme as a four-manifold with corners. Ramanujan J. 20 (3), pp. 409–439.
  • 9: Bibliography B
  • G. Backenstoss (1970) Pionic atoms. Annual Review of Nuclear and Particle Science 20, pp. 467–508.
  • A. Bañuelos and R. A. Depine (1980) A program for computing the Riemann zeta function for complex argument. Comput. Phys. Comm. 20 (3), pp. 441–445.
  • K. L. Bell and N. S. Scott (1980) Coulomb functions (negative energies). Comput. Phys. Comm. 20 (3), pp. 447–458.
  • W. G. Bickley (1935) Some solutions of the problem of forced convection. Philos. Mag. Series 7 20, pp. 322–343.
  • C. Bingham, T. Chang, and D. Richards (1992) Approximating the matrix Fisher and Bingham distributions: Applications to spherical regression and Procrustes analysis. J. Multivariate Anal. 41 (2), pp. 314–337.
  • 10: 20.7 Identities
    See Lawden (1989, pp. 19–20). …
    §20.7(viii) Transformations of Lattice Parameter
    20.7.28 θ 3 ( z | τ + 1 ) = θ 4 ( z | τ ) ,
    20.7.29 θ 4 ( z | τ + 1 ) = θ 3 ( z | τ ) .
    20.7.34 θ 1 ( z , q 2 ) θ 3 ( z , q 2 ) θ 1 ( z , i q ) = θ 2 ( z , q 2 ) θ 4 ( z , q 2 ) θ 2 ( z , i q ) = i 1 / 4 θ 2 ( 0 , q 2 ) θ 4 ( 0 , q 2 ) 2 .