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31: 9.16 Physical Applications
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►Airy functions are applied in many branches of both classical and quantum physics.
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►The frequent appearances of the Airy functions in both classical and quantum physics is associated with wave equations with turning points, for which asymptotic (WKBJ) solutions are exponential on one side and oscillatory on the other.
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►Other applications appear in the study of instability of Couette flow of an inviscid fluid.
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►The KdV equation and solitons have applications in many branches of physics, including plasma physics lattice dynamics, and quantum mechanics.
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►Solutions of the Schrödinger equation involving the Airy functions are given for other potentials in Vallée and Soares (2010).
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32: 2.3 Integrals of a Real Variable
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2.3.3
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►For other examples, see Wong (1989, Chapter 1).
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►Other types of singular behavior in the integrand can be treated in an analogous manner.
…(In other words, differentiation of (2.3.8) with respect to the parameter (or ) is legitimate.)
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►For other estimates of the error term see Lyness (1971).
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33: 22.14 Integrals
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22.14.1
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►The branches of the inverse trigonometric functions are chosen so that they are continuous.
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22.14.4
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►Again, the branches of the inverse trigonometric functions must be continuous.
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§22.14(iii) Other Indefinite Integrals
…34: 10.17 Asymptotic Expansions for Large Argument
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►where the branch of is determined by
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10.17.7
►Corresponding expansions for other ranges of can be obtained by combining (10.17.3), (10.17.5), (10.17.6) with the continuation formulas (10.11.1), (10.11.3), (10.11.4) (or (10.11.7), (10.11.8)), and also the connection formula given by the second of (10.4.4).
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35: 3.10 Continued Fractions
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►However, other continued fractions with the same limit may converge in a much larger domain of the complex plane than the fraction given by (3.10.4) and (3.10.5).
For example, by converting the Maclaurin expansion of (4.24.3), we obtain a continued fraction with the same region of convergence (, ), whereas the continued fraction (4.25.4) converges for all except on the branch cuts from to and to .
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36: 24.16 Generalizations
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24.16.4
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►For this and other properties see Milne-Thomson (1933, pp. 126–153) or Nörlund (1924, pp. 144–162).
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24.16.5
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§24.16(iii) Other Generalizations
►In no particular order, other generalizations include: Bernoulli numbers and polynomials with arbitrary complex index (Butzer et al. (1992)); Euler numbers and polynomials with arbitrary complex index (Butzer et al. (1994)); q-analogs (Carlitz (1954a), Andrews and Foata (1980)); conjugate Bernoulli and Euler polynomials (Hauss (1997, 1998)); Bernoulli–Hurwitz numbers (Katz (1975)); poly-Bernoulli numbers (Kaneko (1997)); Universal Bernoulli numbers (Clarke (1989)); -adic integer order Bernoulli numbers (Adelberg (1996)); -adic -Bernoulli numbers (Kim and Kim (1999)); periodic Bernoulli numbers (Berndt (1975b)); cotangent numbers (Girstmair (1990b)); Bernoulli–Carlitz numbers (Goss (1978)); Bernoulli–Padé numbers (Dilcher (2002)); Bernoulli numbers belonging to periodic functions (Urbanowicz (1988)); cyclotomic Bernoulli numbers (Girstmair (1990a)); modified Bernoulli numbers (Zagier (1998)); higher-order Bernoulli and Euler polynomials with multiple parameters (Erdélyi et al. (1953a, §§1.13.1, 1.14.1)).37: 32.9 Other Elementary Solutions
38: 4.9 Continued Fractions
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4.9.1
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4.9.2
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►For other continued fractions involving logarithms see Lorentzen and Waadeland (1992, pp. 566–568).
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►For other continued fractions involving the exponential function see Lorentzen and Waadeland (1992, pp. 563–564).
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39: 19.9 Inequalities
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19.9.2
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19.9.3
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19.9.5
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►Other inequalities are:
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►Other inequalities for can be obtained from inequalities for given in Carlson (1966, (2.15)) and Carlson (1970) via (19.25.5).