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31: 3.4 Differentiation
3.4.17 1 k ! f ( k ) ( x 0 ) = 1 2 π i C f ( ζ ) ( ζ x 0 ) k + 1 d ζ ,
where C is a simple closed contour described in the positive rotational sense such that C and its interior lie in the domain of analyticity of f , and x 0 is interior to C . …
32: 10.74 Methods of Computation
If values of the Bessel functions J ν ( z ) , Y ν ( z ) , or the other functions treated in this chapter, are needed for integer-spaced ranges of values of the order ν , then a simple and powerful procedure is provided by recurrence relations typified by the first of (10.6.1). …
33: 25.15 Dirichlet L -functions
For the principal character χ 1 ( mod k ) , L ( s , χ 1 ) is analytic everywhere except for a simple pole at s = 1 with residue ϕ ( k ) / k , where ϕ ( k ) is Euler’s totient function (§27.2). …
34: 3.7 Ordinary Differential Equations
For applications to special functions f , g , and h are often simple rational functions. … The eigenvalues λ k are simple, that is, there is only one corresponding eigenfunction (apart from a normalization factor), and when ordered increasingly the eigenvalues satisfy …
35: 22.4 Periods, Poles, and Zeros
Then: (a) In any lattice unit cell p q ( z , k ) has a simple zero at z = p and a simple pole at z = q . …
36: 23.2 Definitions and Periodic Properties
The poles of ( z ) are double with residue 0 ; the poles of ζ ( z ) are simple with residue 1 . The function σ ( z ) is entire and odd, with simple zeros at the lattice points. …
37: 29.12 Definitions
The polynomial P ( ξ ) is of degree n and has m zeros (all simple) in ( 0 , 1 ) and n m zeros (all simple) in ( 1 , k 2 ) . …
38: Bibliography R
  • J. Rushchitsky and S. Rushchitska (2000) On Simple Waves with Profiles in the form of some Special Functions—Chebyshev-Hermite, Mathieu, Whittaker—in Two-phase Media. In Differential Operators and Related Topics, Vol. I (Odessa, 1997), Operator Theory: Advances and Applications, Vol. 117, pp. 313–322.
  • 39: 2.10 Sums and Sequences
    where 𝒞 is a simple closed contour in the annulus that encloses z = 0 . …
    40: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
    For T to be actually self adjoint it is necessary to also show that 𝒟 ( T ) = 𝒟 ( T ) , as it is often the case that T and T have different domains, see Friedman (1990, p 148) for a simple example of such differences involving the differential operator d d x . This question may be rephrased by asking: do f ( x ) and g ( x ) satisfy the same boundary conditions which are needed to fully specify the solutions of a second order linear differential equation? A simple example is the choice f ( a ) = f ( b ) = 0 , and g ( a ) = g ( b ) = 0 , this being only one of many. …
    Example 1: Three Simple Cases where q ( x ) = 0 , X = [ 0 , π ]
    §1.18(vi) Continuous Spectra and Eigenfunction Expansions: Simple Cases
    this being a matrix element of the resolvent F ( T ) = ( z T ) 1 , this being a key quantity in many parts of physics and applied math, quantum scattering theory being a simple example, see Newton (2002, Ch. 7). …