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21: Bibliography
  • M. J. Ablowitz and H. Segur (1977) Exact linearization of a Painlevé transcendent. Phys. Rev. Lett. 38 (20), pp. 1103–1106.
  • A. Adelberg (1992) On the degrees of irreducible factors of higher order Bernoulli polynomials. Acta Arith. 62 (4), pp. 329–342.
  • 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.
  • D. E. Amos (1989) Repeated integrals and derivatives of K Bessel functions. SIAM J. Math. Anal. 20 (1), pp. 169–175.
  • F. M. Arscott (1964a) Integral equations and relations for Lamé functions. Quart. J. Math. Oxford Ser. (2) 15, pp. 103–115.
  • 22: 28.35 Tables
    §28.35 Tables
  • Ince (1932) includes eigenvalues a n , b n , and Fourier coefficients for n = 0 or 1 ( 1 ) 6 , q = 0 ( 1 ) 10 ( 2 ) 20 ( 4 ) 40 ; 7D. Also ce n ( x , q ) , se n ( x , q ) for q = 0 ( 1 ) 10 , x = 1 ( 1 ) 90 , corresponding to the eigenvalues in the tables; 5D. Notation: a n = 𝑏𝑒 n 2 q , b n = 𝑏𝑜 n 2 q .

  • Kirkpatrick (1960) contains tables of the modified functions Ce n ( x , q ) , Se n + 1 ( x , q ) for n = 0 ( 1 ) 5 , q = 1 ( 1 ) 20 , x = 0.1 ( .1 ) 1 ; 4D or 5D.

  • National Bureau of Standards (1967) includes the eigenvalues a n ( q ) , b n ( q ) for n = 0 ( 1 ) 3 with q = 0 ( .2 ) 20 ( .5 ) 37 ( 1 ) 100 , and n = 4 ( 1 ) 15 with q = 0 ( 2 ) 100 ; Fourier coefficients for ce n ( x , q ) and se n ( x , q ) for n = 0 ( 1 ) 15 , n = 1 ( 1 ) 15 , respectively, and various values of q in the interval [ 0 , 100 ] ; joining factors g e , n ( q ) , f e , n ( q ) for n = 0 ( 1 ) 15 with q = 0 ( .5  to  10 ) 100 (but in a different notation). Also, eigenvalues for large values of q . Precision is generally 8D.

  • Zhang and Jin (1996, pp. 521–532) includes the eigenvalues a n ( q ) , b n + 1 ( q ) for n = 0 ( 1 ) 4 , q = 0 ( 1 ) 50 ; n = 0 ( 1 ) 20 ( a ’s) or 19 ( b ’s), q = 1 , 3 , 5 , 10 , 15 , 25 , 50 ( 50 ) 200 . Fourier coefficients for ce n ( x , 10 ) , se n + 1 ( x , 10 ) , n = 0 ( 1 ) 7 . Mathieu functions ce n ( x , 10 ) , se n + 1 ( x , 10 ) , and their first x -derivatives for n = 0 ( 1 ) 4 , x = 0 ( 5 ) 90 . Modified Mathieu functions Mc n ( j ) ( x , 10 ) , Ms n + 1 ( j ) ( x , 10 ) , and their first x -derivatives for n = 0 ( 1 ) 4 , j = 1 , 2 , x = 0 ( .2 ) 4 . Precision is mostly 9S.

  • 23: Software Index
    Open Source With Book Commercial
    20 Theta Functions
    ‘✓’ indicates that a software package implements the functions in a section; ‘a’ indicates available functionality through optional or add-on packages; an empty space indicates no known support. … In the list below we identify four main sources of software for computing special functions. …
  • Commercial Software.

    Such software ranges from a collection of reusable software parts (e.g., a library) to fully functional interactive computing environments with an associated computing language. Such software is usually professionally developed, tested, and maintained to high standards. It is available for purchase, often with accompanying updates and consulting support.

  • The following are web-based software repositories with significant holdings in the area of special functions. …
    24: Bibliography I
  • E. L. Ince (1926) Ordinary Differential Equations. Longmans, Green and Co., London.
  • K. Inkeri (1959) The real roots of Bernoulli polynomials. Ann. Univ. Turku. Ser. A I 37, pp. 1–20.
  • A. Iserles (1996) A First Course in the Numerical Analysis of Differential Equations. Cambridge Texts in Applied Mathematics, No. 15, Cambridge University Press, Cambridge.
  • A. R. Its, A. S. Fokas, and A. A. Kapaev (1994) On the asymptotic analysis of the Painlevé equations via the isomonodromy method. Nonlinearity 7 (5), pp. 1291–1325.
  • A. R. Its and V. Yu. Novokshënov (1986) The Isomonodromic Deformation Method in the Theory of Painlevé Equations. Lecture Notes in Mathematics, Vol. 1191, Springer-Verlag, Berlin.
  • 25: Bibliography M
  • W. Magnus and S. Winkler (1966) Hill’s Equation. Interscience Tracts in Pure and Applied Mathematics, No. 20, Interscience Publishers John Wiley & Sons, New York-London-Sydney.
  • Fr. Mechel (1966) Calculation of the modified Bessel functions of the second kind with complex argument. Math. Comp. 20 (95), pp. 407–412.
  • D. S. Moak (1981) The q -analogue of the Laguerre polynomials. J. Math. Anal. Appl. 81 (1), pp. 20–47.
  • D. Mumford (1984) Tata Lectures on Theta. II. Birkhäuser Boston Inc., Boston, MA.
  • L. A. Muraveĭ (1976) Zeros of the function A i ( z ) σ A i ( z ) . Differential Equations 11, pp. 797–811.
  • 26: 18.40 Methods of Computation
    Usually, however, other methods are more efficient, especially the numerical solution of difference equations3.6) and the application of uniform asymptotic expansions (when available) for OP’s of large degree. … … There are many ways to implement these first two steps, noting that the expressions for α n and β n of equation (18.2.30) are of little practical numerical value, see Gautschi (2004) and Golub and Meurant (2010). … Results of low ( 2 to 3 decimal digits) precision for w ( x ) are easily obtained for N 10 to 20 . … Equation (18.40.7) provides step-histogram approximations to a x d μ ( x ) , as shown in Figure 18.40.1 for N = 12 and 120 , shown here for the repulsive Coulomb–Pollaczek OP’s of Figure 18.39.2, with the parameters as listed therein. …
    27: 30.9 Asymptotic Approximations and Expansions
    §30.9 Asymptotic Approximations and Expansions
    §30.9(i) Prolate Spheroidal Wave Functions
    §30.9(ii) Oblate Spheroidal Wave Functions
    §30.9(iii) Other Approximations and Expansions
    28: 7.8 Inequalities
    §7.8 Inequalities
    7.8.5 x 2 2 x 2 + 1 x 2 ( 2 x 2 + 5 ) 4 x 4 + 12 x 2 + 3 x 𝖬 ( x ) < 2 x 4 + 9 x 2 + 4 4 x 4 + 20 x 2 + 15 < x 2 + 1 2 x 2 + 3 , x 0 .
    7.8.7 sinh x 2 x < e x 2 F ( x ) = 0 x e t 2 d t < e x 2 1 x , x > 0 .
    The function F ( x ) / 1 e 2 x 2 is strictly decreasing for x > 0 . …
    7.8.8 erf x < 1 e 4 x 2 / π , x > 0 .
    29: 20.11 Generalizations and Analogs
    §20.11 Generalizations and Analogs
    The first of equations (20.9.2) can also be written …
    §20.11(iv) Theta Functions with Characteristics
    The importance of these combined theta functions is that sets of twelve equations for the theta functions often can be replaced by corresponding sets of three equations of the combined theta functions, plus permutation symmetry. Such sets of twelve equations include derivatives, differential equations, bisection relations, duplication relations, addition formulas (including new ones for theta functions), and pseudo-addition formulas. …
    30: 18.39 Applications in the Physical Sciences
    also controls time evolution of the wave function Ψ ( x , t ) via the time-dependent Schrödinger equation, … Substitution of (18.39.24) into (18.39.23) then gives the ordinary differential equation for the radial wave function R n , l ( r ) , … The non-relativistic Schrödinger equation describing a single, bound (negative energy) electron, in an L 2 eigenstate of energy E is: … The functions ψ p , l ( r ) satisfy the equation, …
    Discretized and Continuum Expansions of Scattering Eigenfunctions in terms of Pollaczek Polynomials: J-matrix Theory