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31: 10.2 Definitions
§10.2(i) Bessel’s Equation
This differential equation has a regular singularity at z = 0 with indices ± ν , and an irregular singularity at z = of rank 1 ; compare §§2.7(i) and 2.7(ii). …
32: 31.3 Basic Solutions
In general, one of them has a logarithmic singularity at z = 0 .
§31.3(ii) Fuchs–Frobenius Solutions at Other Singularities
Solutions (31.3.1) and (31.3.5)–(31.3.11) comprise a set of 8 local solutions of (31.2.1): 2 per singular point. …
33: Bibliography
  • A. R. Ahmadi and S. E. Widnall (1985) Unsteady lifting-line theory as a singular-perturbation problem. J. Fluid Mech 153, pp. 59–81.
  • H. H. Aly, H. J. W. Müller-Kirsten, and N. Vahedi-Faridi (1975) Scattering by singular potentials with a perturbation – Theoretical introduction to Mathieu functions. J. Mathematical Phys. 16, pp. 961–970.
  • V. I. Arnol’d, S. M. Guseĭn-Zade, and A. N. Varchenko (1988) Singularities of Differentiable Maps. Vol. II. Birkhäuser, Boston-Berlin.
  • 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).
  • J. Avron and B. Simon (1982) Singular Continuous Spectrum for a Class of Almost Periodic Jacobi Matrices. Bulletin of the American Mathematical Society 6 (1), pp. 81–85.
  • 34: 15.19 Methods of Computation
    However, since the growth near the singularities of the differential equation is algebraic rather than exponential, the resulting instabilities in the numerical integration might be tolerable in some cases. …
    35: 21.7 Riemann Surfaces
    This compact curve may have singular points, that is, points at which the gradient of P ~ vanishes. Removing the singularities of this curve gives rise to a two-dimensional connected manifold with a complex-analytic structure, that is, a Riemann surface. All compact Riemann surfaces can be obtained this way.On this surface, we choose 2 g cycles (that is, closed oriented curves, each with at most a finite number of singular points) a j , b j , j = 1 , 2 , , g , such that their intersection indices satisfy … Thus the differentials ω j , j = 1 , 2 , , g have no singularities on Γ . …
    36: 33.2 Definitions and Basic Properties
    §33.2(i) Coulomb Wave Equation
    This differential equation has a regular singularity at ρ = 0 with indices + 1 and , and an irregular singularity of rank 1 at ρ = (§§2.7(i), 2.7(ii)). …
    37: 33.14 Definitions and Basic Properties
    §33.14(i) Coulomb Wave Equation
    Again, there is a regular singularity at r = 0 with indices + 1 and , and an irregular singularity of rank 1 at r = . …
    38: 31.11 Expansions in Series of Hypergeometric Functions
    and (31.11.1) converges to (31.3.10) outside the ellipse in the z -plane with foci at 0, 1, and passing through the third finite singularity at z = a . Every Heun function (§31.4) can be represented by a series of Type I convergent in the whole plane cut along a line joining the two singularities of the Heun function. … The expansion (31.11.1) with (31.11.12) is convergent in the plane cut along the line joining the two singularities z = 0 and z = 1 . …
    39: Bibliography S
  • A. Sidi (2004) Euler-Maclaurin expansions for integrals with endpoint singularities: A new perspective. Numer. Math. 98 (2), pp. 371–387.
  • A. Sidi (2010) A simple approach to asymptotic expansions for Fourier integrals of singular functions. Appl. Math. Comput. 216 (11), pp. 3378–3385.
  • A. Sidi (2012a) Euler-Maclaurin expansions for integrals with arbitrary algebraic endpoint singularities. Math. Comp. 81 (280), pp. 2159–2173.
  • A. Sidi (2012b) Euler-Maclaurin expansions for integrals with arbitrary algebraic-logarithmic endpoint singularities. Constr. Approx. 36 (3), pp. 331–352.
  • B. Simon (1995) Operators with Singular Continuous Spectrum: I. General Operators. Annals of Mathematics 141 (1), pp. 131–145.
  • 40: 15.10 Hypergeometric Differential Equation
    It has regular singularities at z = 0 , 1 , , with corresponding exponent pairs { 0 , 1 c } , { 0 , c a b } , { a , b } , respectively. …They are also numerically satisfactory (§2.7(iv)) in the neighborhood of the corresponding singularity.
    Singularity z = 0
    Singularity z = 1
    Singularity z =