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1: William P. Reinhardt
Reinhardt firmly believes that the Mandelbrot set is a special function, and notes with interest that the natural boundaries of analyticity of many “more normal” special functions are also fractals. …
  • In November 2015, Reinhardt was named Senior Associate Editor of the DLMF and Associate Editor for Chapters 20, 22, and 23.
    2: 33.13 Complex Variable and Parameters
    33.13.1 C ( η ) = 2 e i σ ( η ) ( π η / 2 ) Γ ( + 1 i η ) / Γ ( 2 + 2 ) ,
    33.13.2 R = ( 2 + 1 ) C ( η ) / C 1 ( η ) .
    3: 24.20 Tables
    Wagstaff (1978) gives complete prime factorizations of N n and E n for n = 20 ( 2 ) 60 and n = 8 ( 2 ) 42 , respectively. In Wagstaff (2002) these results are extended to n = 60 ( 2 ) 152 and n = 40 ( 2 ) 88 , respectively, with further complete and partial factorizations listed up to n = 300 and n = 200 , respectively. …
    4: Bibliography
  • A. G. Adams (1969) Algorithm 39: Areas under the normal curve. The Computer Journal 12 (2), pp. 197–198.
  • A. Adelberg (1992) On the degrees of irreducible factors of higher order Bernoulli polynomials. Acta Arith. 62 (4), pp. 329–342.
  • V. I. Arnol’d (1972) Normal forms of functions near degenerate critical points, the Weyl groups A k , D k , E k and Lagrangian singularities. Funkcional. Anal. i Priložen. 6 (4), pp. 3–25 (Russian).
  • V. I. Arnol’d (1974) Normal forms of functions in the neighborhood of degenerate critical points. Uspehi Mat. Nauk 29 (2(176)), pp. 11–49 (Russian).
  • V. I. Arnol’d (1975) Critical points of smooth functions, and their normal forms. Uspehi Mat. Nauk 30 (5(185)), pp. 3–65 (Russian).
  • 5: 28.5 Second Solutions fe n , ge n
    28.5.1 fe n ( z , q ) = C n ( q ) ( z ce n ( z , q ) + f n ( z , q ) ) ,
    The factors C n ( q ) and S n ( q ) in (28.5.1) and (28.5.2) are normalized so that
    28.5.5 ( C n ( q ) ) 2 0 2 π ( f n ( x , q ) ) 2 d x = ( S n ( q ) ) 2 0 2 π ( g n ( x , q ) ) 2 d x = π .
    (Other normalizations for C n ( q ) and S n ( q ) can be found in the literature, but most formulas—including connection formulas—are unaffected since fe n ( z , q ) / C n ( q ) and ge n ( z , q ) / S n ( q ) are invariant.) … As a consequence of the factor z on the right-hand sides of (28.5.1), (28.5.2), all solutions of Mathieu’s equation that are linearly independent of the periodic solutions are unbounded as z ± on . …
    6: 18.39 Applications in the Physical Sciences
    All are written in the same form as the product of three factors: the square root of a weight function w ( x ) , the corresponding OP or EOP, and constant factors ensuring unit normalization. … By Table 18.3.1#12 the normalized stationary states and corresponding eigenvalues are …With the normalization factor ( c h n ) 1 / 2 the ψ n are orthonormal in L 2 ( , d x ) . … There is no need for a normalization constant here, as appropriate constants already appear in §18.36(vi). … Explicit normalization is given for the second, third, and fourth of these, paragraphs c) and d), below. …
    7: 28.12 Definitions and Basic Properties
    In consequence, for the Floquet solutions w ( z ) the factor e π i ν in (28.2.14) is no longer ± 1 . …
    28.12.2 λ ν ( q ) = λ ν ( q ) = λ ν ( q ) .
    As in §28.7 values of q for which (28.2.16) has simple roots λ are called normal values with respect to ν . For real values of ν and q all the λ ν ( q ) are real, and q is normal. … If q is a normal value of the corresponding equation (28.2.16), then these functions are uniquely determined as analytic functions of z and q by the normalization
    8: 3.6 Linear Difference Equations
    It therefore remains to apply a normalizing factor Λ . The process is then repeated with a higher value of N , and the normalized solutions compared. … The normalizing factor Λ can be the true value of w 0 divided by its trial value, or Λ can be chosen to satisfy a known property of the wanted solution of the form … … For further information, including a more general form of normalizing condition, other examples, convergence proofs, and error analyses, see Olver (1967a), Olver and Sookne (1972), and Wimp (1984, Chapter 6). …
    9: Bibliography B
  • G. Backenstoss (1970) Pionic atoms. Annual Review of Nuclear and Particle Science 20, pp. 467–508.
  • P. A. Becker (1997) Normalization integrals of orthogonal Heun functions. J. Math. Phys. 38 (7), pp. 3692–3699.
  • S. L. Belousov (1962) Tables of Normalized Associated Legendre Polynomials. Pergamon Press, The Macmillan Co., Oxford-New York.
  • E. Berti and V. Cardoso (2006) Quasinormal ringing of Kerr black holes: The excitation factors. Phys. Rev. D 74 (104020), pp. 1–27.
  • D. M. Bressoud (1989) Factorization and Primality Testing. Springer-Verlag, New York.
  • 10: 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.
  • N. Kimura (1988) On the degree of an irreducible factor of the Bernoulli polynomials. Acta Arith. 50 (3), pp. 243–249.
  • 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.
  • S. Koizumi (1976) Theta relations and projective normality of Abelian varieties. Amer. J. Math. 98 (4), pp. 865–889.