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asymptotic forms of higher coefficients

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1: 28.4 Fourier Series
§28.4(vii) Asymptotic Forms for Large m
2: 2.9 Difference Equations
Formal solutions are … c 0 = 1 , and higher coefficients are determined by formal substitution. … with a 0 , j = 1 and higher coefficients given by (2.9.7) (in the present case the coefficients of a s , j and a s 1 , j are zero). … For analogous results for difference equations of the form
3: 28.15 Expansions for Small q
§28.15 Expansions for Small q
28.15.1 λ ν ( q ) = ν 2 + 1 2 ( ν 2 1 ) q 2 + 5 ν 2 + 7 32 ( ν 2 1 ) 3 ( ν 2 4 ) q 4 + 9 ν 4 + 58 ν 2 + 29 64 ( ν 2 1 ) 5 ( ν 2 4 ) ( ν 2 9 ) q 6 + .
Higher coefficients can be found by equating powers of q in the following continued-fraction equation, with a = λ ν ( q ) : …
4: 8.11 Asymptotic Approximations and Expansions
§8.11 Asymptotic Approximations and Expansions
For an exponentially-improved asymptotic expansion (§2.11(iii)) see Olver (1991a). … where … See Tricomi (1950b) for these approximations, together with higher terms and extensions to complex variables. …
5: 2.11 Remainder Terms; Stokes Phenomenon
with … For higher-order Stokes phenomena see Olde Daalhuis (2004b) and Howls et al. (2004). … For higher-order differential equations, see Olde Daalhuis (1998a, b). … Furthermore, on proceeding to higher values of n with higher precision, much more accuracy is achievable. … Their extrapolation is based on assumed forms of remainder terms that may not always be appropriate for asymptotic expansions. …
6: 2.4 Contour Integrals
§2.4(i) Watson’s Lemma
For examples see Olver (1997b, pp. 315–320). … The final expansion then has the formHigher coefficients b 2 s in (2.4.15) can be found from (2.3.18) with λ = 1 , μ = 2 , and s replaced by 2 s . … For a symbolic method for evaluating the coefficients in the asymptotic expansions see Vidūnas and Temme (2002). …
7: 9.7 Asymptotic Expansions
§9.7 Asymptotic Expansions
§9.7(iii) Error Bounds for Real Variables
Corresponding bounds for the errors in (9.7.7) to (9.7.14) may be obtained by use of these results and those of §9.2(v) and their differentiated forms. … For higher re-expansions of the remainder terms see Olde Daalhuis (1995, 1996), and Olde Daalhuis and Olver (1995a).
8: 3.6 Linear Difference Equations
Many special functions satisfy second-order recurrence relations, or difference equations, of the formThe values of w N and w N + 1 needed to begin the backward recursion may be available, for example, from asymptotic expansions (§2.9). … The process is then repeated with a higher value of N , and the normalized solutions compared. … The normalizing factor Λ can be the true value of w 0 divided by its trial value, or Λ can be chosen to satisfy a known property of the wanted solution of the formFor further information, including a more general form of normalizing condition, other examples, convergence proofs, and error analyses, see Olver (1967a), Olver and Sookne (1972), and Wimp (1984, Chapter 6). …
9: Bibliography R
  • M. Rahman (1981) A non-negative representation of the linearization coefficients of the product of Jacobi polynomials. Canad. J. Math. 33 (4), pp. 915–928.
  • W. H. Reid (1974a) Uniform asymptotic approximations to the solutions of the Orr-Sommerfeld equation. I. Plane Couette flow. Studies in Appl. Math. 53, pp. 91–110.
  • È. Ya. Riekstynš (1991) Asymptotics and Bounds of the Roots of Equations (Russian). Zinatne, Riga.
  • W. Rudin (1973) Functional Analysis. McGraw-Hill Book Co., New York.
  • 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.
  • 10: Bibliography
  • A. Adelberg (1992) On the degrees of irreducible factors of higher order Bernoulli polynomials. Acta Arith. 62 (4), pp. 329–342.
  • T. M. Apostol (1985a) Formulas for higher derivatives of the Riemann zeta function. Math. Comp. 44 (169), pp. 223–232.
  • V. I. Arnol’d (1975) Critical points of smooth functions, and their normal forms. Uspehi Mat. Nauk 30 (5(185)), pp. 3–65 (Russian).
  • G. Arutyunov and M. Staudacher (2004) Matching higher conserved charges for strings and spins. J. High Energy Phys. 2004 (3).
  • R. Askey (1982a) Commentary on the Paper “Beiträge zur Theorie der Toeplitzschen Form. In Gábor Szegő, Collected Papers. Vol. 1, Contemporary Mathematicians, pp. 303–305.