Stokes phenomenon
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1—10 of 12 matching pages
1: 7.20 Mathematical Applications
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►For applications of the complementary error function in uniform asymptotic approximations of integrals—saddle point coalescing with a pole or saddle point coalescing with an endpoint—see Wong (1989, Chapter 7), Olver (1997b, Chapter 9), and van der Waerden (1951).
►The complementary error function also plays a ubiquitous role in constructing exponentially-improved asymptotic expansions and providing a smooth interpretation of the Stokes phenomenon; see §§2.11(iii) and 2.11(iv).
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2: 8.22 Mathematical Applications
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8.22.1
►plays a fundamental role in re-expansions of remainder terms in asymptotic expansions, including exponentially-improved expansions and a smooth interpretation of the Stokes phenomenon.
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3: Bibliography P
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Stokes phenomenon demystified.
Bull. Inst. Math. Appl. 31 (1-2), pp. 21–28.
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Smoothing of the Stokes phenomenon for high-order differential equations.
Proc. Roy. Soc. London Ser. A 436, pp. 165–186.
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Smoothing of the Stokes phenomenon using Mellin-Barnes integrals.
J. Comput. Appl. Math. 41 (1-2), pp. 117–133.
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The Stokes phenomenon associated with the Hurwitz zeta function
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Proc. Roy. Soc. London Ser. A 461, pp. 297–304.
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The Stokes phenomenon and the Lerch zeta function.
Mathematica Aeterna 6 (2), pp. 181–196.
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4: 2.11 Remainder Terms; Stokes Phenomenon
§2.11 Remainder Terms; Stokes Phenomenon
… ►§2.11(iv) Stokes Phenomenon
… ►That the change in their forms is discontinuous, even though the function being approximated is analytic, is an example of the Stokes phenomenon. Where should the change-over take place? Can it be accomplished smoothly? …5: 10.46 Generalized and Incomplete Bessel Functions; Mittag-Leffler Function
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►For exponentially-improved asymptotic expansions in the same circumstances, together with smooth interpretations of the corresponding Stokes phenomenon (§§2.11(iii)–2.11(v)) see Wong and Zhao (1999b) when , and Wong and Zhao (1999a) when .
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6: Bibliography I
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Quasi-linear Stokes phenomenon for the second Painlevé transcendent.
Nonlinearity 16 (1), pp. 363–386.
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7: 7.12 Asymptotic Expansions
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►For these and other error bounds see Olver (1997b, pp. 109–112), with and replaced by ; compare (7.11.2).
►For re-expansions of the remainder terms leading to larger sectors of validity, exponential improvement, and a smooth interpretation of the Stokes phenomenon, see §§2.11(ii)–2.11(iv) and use (7.11.3).
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8: Bibliography K
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Essential singularity of the Painlevé function of the second kind and the nonlinear Stokes phenomenon.
Zap. Nauchn. Sem. Leningrad. Otdel. Mat. Inst. Steklov.
(LOMI) 187, pp. 139–170 (Russian).
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Quasi-linear Stokes phenomenon for the Painlevé first equation.
J. Phys. A 37 (46), pp. 11149–11167.
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9: 6.12 Asymptotic Expansions
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►For re-expansions of the remainder term leading to larger sectors of validity, exponential improvement, and a smooth interpretation of the Stokes phenomenon, see §§2.11(ii)–2.11(iv), with .
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10: Bibliography H
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On the higher-order Stokes phenomenon.
Proc. Roy. Soc. London Ser. A 460, pp. 2285–2303.
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