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11: 18.39 Applications in the Physical Sciences
c) A Rational SUSY Potential argument
12: 18.36 Miscellaneous Polynomials
In §18.39(i) it is seen that the functions, w ( x ) H ^ n + 3 ( x ) , are solutions of a Schrödinger equation with a rational potential energy; and, in spite of first appearances, the Sturm oscillation theorem, Simon (2005c, Theorem 3.3, p. 35), is satisfied. …
13: 28.12 Definitions and Basic Properties
When ν = s / m is a rational number, but not an integer, all solutions of Mathieu’s equation are periodic with period 2 m π . …
14: 3.7 Ordinary Differential Equations
For applications to special functions f , g , and h are often simple rational functions. … For general information on solutions of equation (3.7.1) see §1.13. …
§3.7(ii) Taylor-Series Method: Initial-Value Problems
The Sturm–Liouville eigenvalue problem is the construction of a nontrivial solution of the system …
15: 3.11 Approximation Techniques
§3.11(iii) Minimax Rational Approximations
Then the minimax (or best uniform) rational approximation …
Example
The rational function …
16: 31.8 Solutions via Quadratures
By automorphisms from §31.2(v), similar solutions also exist for m 0 , m 1 , m 2 , m 3 , and Ψ g , N ( λ , z ) may become a rational function in z . …
17: 32.2 Differential Equations
The six equations are sometimes referred to as the Painlevé transcendents, but in this chapter this term will be used only for their solutions. … be a nonlinear second-order differential equation in which F is a rational function of w and d w / d z , and is locally analytic in z , that is, analytic except for isolated singularities in . In general the singularities of the solutions are movable in the sense that their location depends on the constants of integration associated with the initial or boundary conditions. An equation is said to have the Painlevé property if all its solutions are free from movable branch points; the solutions may have movable poles or movable isolated essential singularities (§1.10(iii)), however. … Let …
18: 32.10 Special Function Solutions
§32.10 Special Function Solutions
where F j ( w , z ) is polynomial in w with coefficients that are rational functions of z . … with solutionwhich has the solution
19: Bibliography B
  • A. P. Bassom, P. A. Clarkson, C. K. Law, and J. B. McLeod (1998) Application of uniform asymptotics to the second Painlevé transcendent. Arch. Rational Mech. Anal. 143 (3), pp. 241–271.
  • W. G. Bickley (1935) Some solutions of the problem of forced convection. Philos. Mag. Series 7 20, pp. 322–343.
  • J. M. Blair, C. A. Edwards, and J. H. Johnson (1976) Rational Chebyshev approximations for the inverse of the error function. Math. Comp. 30 (136), pp. 827–830.
  • J. M. Blair, C. A. Edwards, and J. H. Johnson (1978) Rational Chebyshev approximations for the Bickley functions K i n ( x ) . Math. Comp. 32 (143), pp. 876–886.
  • J. M. Borwein and I. J. Zucker (1992) Fast evaluation of the gamma function for small rational fractions using complete elliptic integrals of the first kind. IMA J. Numer. Anal. 12 (4), pp. 519–526.
  • 20: Bibliography S
  • H. Sakai (2001) Rational surfaces associated with affine root systems and geometry of the Painlevé equations. Comm. Math. Phys. 220 (1), pp. 165–229.
  • T. Schmelzer and L. N. Trefethen (2007) Computing the gamma function using contour integrals and rational approximations. SIAM J. Numer. Anal. 45 (2), pp. 558–571.
  • J. H. Silverman and J. Tate (1992) Rational Points on Elliptic Curves. Undergraduate Texts in Mathematics, Springer-Verlag, New York.
  • R. Spigler (1984) The linear differential equation whose solutions are the products of solutions of two given differential equations. J. Math. Anal. Appl. 98 (1), pp. 130–147.
  • A. J. Stone and C. P. Wood (1980) Root-rational-fraction package for exact calculation of vector-coupling coefficients. Comput. Phys. Comm. 21 (2), pp. 195–205.