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31—40 of 68 matching pages

31: 31.17 Physical Applications
32: Bibliography O
  • M. K. Ong (1986) A closed form solution of the s -wave Bethe-Goldstone equation with an infinite repulsive core. J. Math. Phys. 27 (4), pp. 1154–1158.
  • 33: 30.6 Functions of Complex Argument
    34: 20.13 Physical Applications
    This allows analytic time propagation of quantum wave-packets in a box, or on a ring, as closed-form solutions of the time-dependent Schrödinger equation.
    35: 30.9 Asymptotic Approximations and Expansions
    36: Bibliography K
  • M. D. Kruskal (1974) The Korteweg-de Vries Equation and Related Evolution Equations. In Nonlinear Wave Motion (Proc. AMS-SIAM Summer Sem., Clarkson Coll. Tech., Potsdam, N.Y., 1972), A. C. Newell (Ed.), Lectures in Appl. Math., Vol. 15, pp. 61–83.
  • 37: 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 ) , … (where the minus sign is often omitted, as it arises as an arbitrary phase when taking the square root of the real, positive, norm of the wave function), allowing equation (18.39.37) to be rewritten in terms of the associated Coulomb–Laguerre polynomials 𝐋 n + l 2 l + 1 ( ρ n ) . …
    Discretized and Continuum Expansions of Scattering Eigenfunctions in terms of Pollaczek Polynomials: J-matrix Theory
    38: 30.12 Generalized and Coulomb Spheroidal Functions
    Generalized spheroidal wave functions and Coulomb spheroidal functions are solutions of the differential equation
    39: 28.31 Equations of Whittaker–Hill and Ince
    §28.31 Equations of Whittaker–Hill and Ince
    §28.31(iii) Paraboloidal Wave Functions
    With (28.31.10) and (28.31.11), …are called paraboloidal wave functions. …
    Asymptotic Behavior
    40: 31.18 Methods of Computation
    The computation of the accessory parameter for the Heun functions is carried out via the continued-fraction equations (31.4.2) and (31.11.13) in the same way as for the Mathieu, Lamé, and spheroidal wave functions in Chapters 2830.