large a %28or b%29 and c
(0.004 seconds)
21—30 of 34 matching pages
21: Bibliography W
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Asymptotische Entwicklungen der hypergeometrischen Funktion für und konstante Werte und
.
Demonstratio Math. 21 (2), pp. 441–458 (German).
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Hill’s equation with a large potential.
SIAM J. Appl. Math. 45 (2), pp. 200–214.
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Wave functions for large arguments by the amplitude-phase method.
Phys. Rev. 52, pp. 1123–1127.
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An asymptotic expansion of with large variable and parameters.
Math. Comp. 27 (122), pp. 429–436.
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Spin-spin correlation functions for the two-dimensional Ising model: Exact theory in the scaling region.
Phys. Rev. B 13, pp. 316–374.
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22: Bibliography D
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Sur une classe de nombres rationnels réductibles aux nombres de Bernoulli.
Bull. Sci. Math. (2) 28, pp. 29–32 (French).
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Computing Riemann matrices of algebraic curves.
Phys. D 152/153, pp. 28–46.
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Note on the addition theorem of parabolic cylinder functions.
J. Indian Math. Soc. (N. S.) 4, pp. 29–30.
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Conical functions with one or both parameters large.
Proc. Roy. Soc. Edinburgh Sect. A 119 (3-4), pp. 311–327.
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The incomplete beta function—a historical profile.
Arch. Hist. Exact Sci. 24 (1), pp. 11–29.
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23: Mathematical Introduction
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βΊSee, for example, Chapters 16, 17, 18, 19, 21, 27, 29, 31, 32, 34, 35, and 36.
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βΊFirst, the editors instituted a validation process for the whole technical content of each chapter.
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βΊFor example, for the hypergeometric function we often use the notation (§15.2(i)) in place of the more conventional or .
This is because is akin to the notation used for Bessel functions (§10.2(ii)), inasmuch as is an entire function of each of its parameters , , and :β this results in fewer restrictions and simpler equations.
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βΊOther examples are: (a) the notation for the Ferrers functions—also known as associated Legendre functions on the cut—for which existing notations can easily be confused with those for other associated Legendre functions (§14.1); (b) the spherical Bessel functions for which existing notations are unsymmetric and inelegant (§§10.47(i) and 10.47(ii)); and (c) elliptic integrals for which both Legendre’s forms and the more recent symmetric forms are treated fully (Chapter 19).
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24: Bibliography E
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The penetration of a potential barrier by electrons.
Phys. Rev. 35 (11), pp. 1303–1309.
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Properties of a Raman atom-laser output coupler.
J. Phys. B 32 (12), pp. 2935–2950.
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A formula including Legendre’s
.
Messenger of Math. 33, pp. 31–32.
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Higher Transcendental Functions. Vol. II.
McGraw-Hill Book Company, Inc., New York-Toronto-London.
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Painlevé transcendent describes quantum correlation function of the antiferromagnet away from the free-fermion point.
J. Phys. A 29 (17), pp. 5619–5626.
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25: 26.12 Plane Partitions
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βΊWe define the
box
as
…Then the number of plane partitions in is
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βΊThe number of symmetric plane partitions in is
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βΊThe complement of is .
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βΊThe number of descending plane partitions in is
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26: Bibliography U
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βΊ
On Kelvin’s ship-wave pattern.
J. Fluid Mech. 8 (3), pp. 418–431.
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Integrals with a large parameter. Several nearly coincident saddle-points.
Proc. Cambridge Philos. Soc. 72, pp. 49–65.
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Integrals with a large parameter: A double complex integral with four nearly coincident saddle-points.
Math. Proc. Cambridge Philos. Soc. 87 (2), pp. 249–273.
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Integrals with a large parameter: Legendre functions of large degree and fixed order.
Math. Proc. Cambridge Philos. Soc. 95 (2), pp. 367–380.
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Theory of the Whittaker-Hill equation.
Proc. Roy. Soc. Edinburgh Sect. A 69, pp. 28–44.
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27: Bibliography Y
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Generalized Hypergeometric Functions and Laguerre Polynomials in Two Variables.
In Hypergeometric Functions on Domains of Positivity, Jack
Polynomials, and Applications (Tampa, FL, 1991),
Contemporary Mathematics, Vol. 138, pp. 239–259.
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Computation of the derivatives of the Riemann zeta-function in the complex domain.
USSR Comput. Math. and Math. Phys. 28 (4), pp. 115–124.
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Software for interval arithmetic: A reasonably portable package.
ACM Trans. Math. Software 5 (1), pp. 50–63.
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Computation of Kummer functions for large argument by using the -method.
Trans. Inform. Process. Soc. Japan 36 (10), pp. 2335–2342 (Japanese).
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Mathematical Apparatus of the Theory of Angular Momentum.
Israel Program for Scientific Translations for National Science
Foundation and the National Aeronautics and Space Administration, Jerusalem.
28: 10.20 Uniform Asymptotic Expansions for Large Order
§10.20 Uniform Asymptotic Expansions for Large Order
… βΊIn the following formulas for the coefficients , , , and , , are the constants defined in §9.7(i), and , are the polynomials in of degree defined in §10.41(ii). … βΊNote: Another way of arranging the above formulas for the coefficients , and would be by analogy with (12.10.42) and (12.10.46). … βΊEach of the coefficients , , , and , , is real and infinitely differentiable on the interval . … βΊFor numerical tables of , and , , , and see Olver (1962, pp. 28–42). …29: 10.21 Zeros
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βΊ
§10.21(vi) McMahon’s Asymptotic Expansions for Large Zeros
… βΊWith , the right-hand side is the asymptotic expansion of for large . … βΊ§10.21(vii) Asymptotic Expansions for Large Order
… βΊ§10.21(viii) Uniform Asymptotic Approximations for Large Order
… βΊ and are defined by (10.20.11) and (10.20.12) with . …30: Bibliography P
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Stokes phenomenon demystified.
Bull. Inst. Math. Appl. 31 (1-2), pp. 21–28.
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Exactification of the method of steepest descents: The Bessel functions of large order and argument.
Proc. Roy. Soc. London Ser. A 460, pp. 2737–2759.
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βΊ
Handbook of the Normal Distribution.
Statistics: Textbooks and Monographs, Vol. 40, Marcel Dekker Inc., New York.
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Algorithm 28. Algorithm for the computation of Bessel function integrals.
J. Comput. Appl. Math. 11 (1), pp. 119–137.
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βΊ
A First Course in Real Analysis.
2nd edition, Undergraduate Texts in Mathematics, Springer-Verlag, New York.
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