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11: Bibliography H
  • J. R. Herndon (1961a) Algorithm 55: Complete elliptic integral of the first kind. Comm. ACM 4 (4), pp. 180.
  • D. R. Herrick and S. O’Connor (1998) Inverse virial symmetry of diatomic potential curves. J. Chem. Phys. 109 (1), pp. 11–19.
  • H. W. Hethcote (1970) Error bounds for asymptotic approximations of zeros of Hankel functions occurring in diffraction problems. J. Mathematical Phys. 11 (8), pp. 2501–2504.
  • G. W. Hill (1970) Algorithm 395: Student’s t-distribution. Comm. ACM 13 (10), pp. 617–619.
  • C. Hunter (1981) Two Parametric Eigenvalue Problems of Differential Equations. In Spectral Theory of Differential Operators (Birmingham, AL, 1981), North-Holland Math. Stud., Vol. 55, pp. 233–241.
  • 12: William P. Reinhardt
    Older work on the scattering theory of the atomic Coulomb problem led to the discovery of new classes of orthogonal polynomials relating to the spectral theory of Schrödinger operators, and new uses of old ones: this work was strongly motivated by his original ownership of a 1964 hard copy printing of the original AMS 55 NBS Handbook of Mathematical Functions. …
    13: Bibliography E
  • C. Eckart (1930) The penetration of a potential barrier by electrons. Phys. Rev. 35 (11), pp. 1303–1309.
  • A. Erdélyi, W. Magnus, F. Oberhettinger, and F. G. Tricomi (1953a) Higher Transcendental Functions. Vol. I. McGraw-Hill Book Company, Inc., New York-Toronto-London.
  • A. Erdélyi, W. Magnus, F. Oberhettinger, and F. G. Tricomi (1953b) Higher Transcendental Functions. Vol. II. McGraw-Hill Book Company, Inc., New York-Toronto-London.
  • L. Euler (1768) Institutiones Calculi Integralis. Opera Omnia (1), Vol. 11, pp. 110–113.
  • G. A. Evans and J. R. Webster (1999) A comparison of some methods for the evaluation of highly oscillatory integrals. J. Comput. Appl. Math. 112 (1-2), pp. 55–69.
  • 14: Bibliography N
  • G. Nemes (2020) An extension of Laplace’s method. Constr. Approx. 51 (2), pp. 247–272.
  • E. Neuman (1969a) Elliptic integrals of the second and third kinds. Zastos. Mat. 11, pp. 99–102.
  • E. Neuman (1969b) On the calculation of elliptic integrals of the second and third kinds. Zastos. Mat. 11, pp. 91–94.
  • C. J. Noble (2004) Evaluation of negative energy Coulomb (Whittaker) functions. Comput. Phys. Comm. 159 (1), pp. 55–62.
  • V. Yu. Novokshënov (1985) The asymptotic behavior of the general real solution of the third Painlevé equation. Dokl. Akad. Nauk SSSR 283 (5), pp. 1161–1165 (Russian).
  • 15: Bibliography
  • M. Abramowitz (1949) Asymptotic expansions of spheroidal wave functions. J. Math. Phys. Mass. Inst. Tech. 28, pp. 195–199.
  • S. Ahmed and M. E. Muldoon (1980) On the zeros of confluent hypergeometric functions. III. Characterization by means of nonlinear equations. Lett. Nuovo Cimento (2) 29 (11), pp. 353–358.
  • F. Alhargan and S. Judah (1995) A general mode theory for the elliptic disk microstrip antenna. IEEE Trans. Antennas and Propagation 43 (6), pp. 560–568.
  • 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).
  • R. Askey and J. Wilson (1985) Some basic hypergeometric orthogonal polynomials that generalize Jacobi polynomials. Mem. Amer. Math. Soc. 54 (319), pp. iv+55.
  • 16: 4.24 Inverse Trigonometric Functions: Further Properties
    4.24.2 arccos z = ( 2 ( 1 z ) ) 1 / 2 ( 1 + n = 1 1 3 5 ( 2 n 1 ) 2 2 n ( 2 n + 1 ) n ! ( 1 z ) n ) , | 1 z | 2 .
    4.24.5 arctan z = z z 2 + 1 ( 1 + 2 3 z 2 1 + z 2 + 2 4 3 5 ( z 2 1 + z 2 ) 2 + ) , ( z 2 ) > 1 2 ,
    4.24.6 x 2 y 2 = 1 2 .
    4.24.14 Arccos u ± Arccos v = Arccos ( u v ( ( 1 u 2 ) ( 1 v 2 ) ) 1 / 2 ) ,
    4.24.16 Arcsin u ± Arccos v = Arcsin ( u v ± ( ( 1 u 2 ) ( 1 v 2 ) ) 1 / 2 ) = Arccos ( v ( 1 u 2 ) 1 / 2 u ( 1 v 2 ) 1 / 2 ) ,
    17: 24.13 Integrals
    For m , n = 1 , 2 , , …
    24.13.9 0 1 / 2 E 2 n ( t ) d t = E 2 n + 1 ( 0 ) 2 n + 1 = 2 ( 2 2 n + 2 1 ) B 2 n + 2 ( 2 n + 1 ) ( 2 n + 2 ) ,
    24.13.10 0 1 / 2 E 2 n 1 ( t ) d t = E 2 n n 2 2 n + 1 , n = 1 , 2 , .
    For m , n = 1 , 2 , , … For other integrals see Prudnikov et al. (1990, pp. 55–57).
    18: Bibliography C
  • M. A. Chaudhry and S. M. Zubair (1994) Generalized incomplete gamma functions with applications. J. Comput. Appl. Math. 55 (1), pp. 99–124.
  • M. Colman, A. Cuyt, and J. Van Deun (2011) Validated computation of certain hypergeometric functions. ACM Trans. Math. Software 38 (2), pp. Art. 11, 20.
  • J. N. L. Connor (1976) Catastrophes and molecular collisions. Molecular Phys. 31 (1), pp. 33–55.
  • F. Cooper, A. Khare, and A. Saxena (2006) Exact elliptic compactons in generalized Korteweg-de Vries equations. Complexity 11 (6), pp. 30–34.
  • A. Csótó and G. M. Hale (1997) S -matrix and R -matrix determination of the low-energy He 5 and Li 5 resonance parameters. Phys. Rev. C 55 (1), pp. 536–539.
  • 19: Bibliography G
  • B. Gambier (1910) Sur les équations différentielles du second ordre et du premier degré dont l’intégrale générale est a points critiques fixes. Acta Math. 33 (1), pp. 1–55.
  • W. Gautschi (1966) Algorithm 292: Regular Coulomb wave functions. Comm. ACM 9 (11), pp. 793–795.
  • A. Gil, J. Segura, and N. M. Temme (2002c) Computing complex Airy functions by numerical quadrature. Numer. Algorithms 30 (1), pp. 11–23.
  • P. Groeneboom and D. R. Truax (2000) A monotonicity property of the power function of multivariate tests. Indag. Math. (N.S.) 11 (2), pp. 209–218.
  • V. I. Gromak (1975) Theory of Painlevé’s equations. Differ. Uravn. 11 (11), pp. 373–376 (Russian).
  • 20: 10.60 Sums
    10.60.11 n = 0 𝗃 n 2 ( z ) = Si ( 2 z ) 2 z .
    10.60.12 n = 0 ( 2 n + 1 ) 𝗃 n 2 ( z ) = 1 ,
    10.60.13 n = 0 ( 1 ) n ( 2 n + 1 ) 𝗃 n 2 ( z ) = sin ( 2 z ) 2 z ,
    For further sums of series of spherical Bessel functions, or modified spherical Bessel functions, see §6.10(ii), Luke (1969b, pp. 55–58), Vavreck and Thompson (1984), Harris (2000), and Rottbrand (2000). … See also Watson (1944, Chapters 11 and 16).