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21: 8.12 Uniform Asymptotic Expansions for Large Parameter
The right-hand sides of equations (8.12.9), (8.12.10) have removable singularities at η = 0 , and the Maclaurin series expansion of c k ( η ) is given by … A different type of uniform expansion with coefficients that do not possess a removable singularity at z = a is given by …
22: 18.40 Methods of Computation
Results similar to these appear in Langhoff et al. (1976) in methods developed for physics applications, and which includes treatments of systems with discontinuities in μ ( x ) , using what is referred to as the Stieltjes derivative which may be traced back to Stieltjes, as discussed by Deltour (1968, Eq. 12). …
23: 28.12 Definitions and Basic Properties
As a function of ν with fixed q ( 0 ), λ ν ( q ) is discontinuous at ν = ± 1 , ± 2 , . …
24: Bibliography D
  • T. M. Dunster (1996b) Asymptotics of the generalized exponential integral, and error bounds in the uniform asymptotic smoothing of its Stokes discontinuities. Proc. Roy. Soc. London Ser. A 452, pp. 1351–1367.
  • 25: 4.37 Inverse Hyperbolic Functions
    26: 3.1 Arithmetics and Error Measures
    During the calculations common divisors are removed from the rational numbers, and the final results can be converted to decimal representations of arbitrary length. …
    27: 11.6 Asymptotic Expansions
    28: 16.5 Integral Representations and Integrals
    In (16.5.3) the restriction z < 1 can be removed when p < q . …
    29: 18.1 Notation
    30: 25.11 Hurwitz Zeta Function
    25.11.36Removed because it is just (25.15.1) combined with (25.15.3).