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21: Bibliography W
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  • E. Wagner (1988) Asymptotische Entwicklungen der hypergeometrischen Funktion F ⁒ ( a , b , c , z ) für | c | und konstante Werte a , b und z . Demonstratio Math. 21 (2), pp. 441–458 (German).
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  • M. I. Weinstein and J. B. Keller (1985) Hill’s equation with a large potential. SIAM J. Appl. Math. 45 (2), pp. 200–214.
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  • J. A. Wheeler (1937) Wave functions for large arguments by the amplitude-phase method. Phys. Rev. 52, pp. 1123–1127.
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  • R. Wong (1973a) An asymptotic expansion of W k , m ⁒ ( z ) with large variable and parameters. Math. Comp. 27 (122), pp. 429–436.
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  • T. T. Wu, B. M. McCoy, C. A. Tracy, and E. Barouch (1976) Spin-spin correlation functions for the two-dimensional Ising model: Exact theory in the scaling region. Phys. Rev. B 13, pp. 316–374.
  • 22: Bibliography D
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  • M. D’Ocagne (1904) Sur une classe de nombres rationnels réductibles aux nombres de Bernoulli. Bull. Sci. Math. (2) 28, pp. 29–32 (French).
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  • B. Deconinck and M. van Hoeij (2001) Computing Riemann matrices of algebraic curves. Phys. D 152/153, pp. 28–46.
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  • S. C. Dhar (1940) Note on the addition theorem of parabolic cylinder functions. J. Indian Math. Soc. (N. S.) 4, pp. 29–30.
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  • T. M. Dunster (1991) Conical functions with one or both parameters large. Proc. Roy. Soc. Edinburgh Sect. A 119 (3-4), pp. 311–327.
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  • J. Dutka (1981) The incomplete beta function—a historical profile. Arch. Hist. Exact Sci. 24 (1), pp. 11–29.
  • 23: Mathematical Introduction
    β–ΊSee, for example, Chapters 16, 17, 18, 19, 21, 27, 29, 31, 32, 34, 35, and 36. … β–ΊFirst, the editors instituted a validation process for the whole technical content of each chapter. … β–ΊFor example, for the hypergeometric function we often use the notation 𝐅 ⁑ ( a , b ; c ; z ) 15.2(i)) in place of the more conventional F 1 2 ⁑ ( a , b ; c ; z ) or F ⁑ ( a , b ; c ; z ) . This is because 𝐅 is akin to the notation used for Bessel functions (§10.2(ii)), inasmuch as 𝐅 is an entire function of each of its parameters a , b , and c :​ this results in fewer restrictions and simpler equations. … β–ΊOther 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). …
    24: Bibliography E
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  • C. Eckart (1930) The penetration of a potential barrier by electrons. Phys. Rev. 35 (11), pp. 1303–1309.
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  • M. Edwards, D. A. Griggs, P. L. Holman, C. W. Clark, S. L. Rolston, and W. D. Phillips (1999) Properties of a Raman atom-laser output coupler. J. Phys. B 32 (12), pp. 2935–2950.
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  • E. B. Elliott (1903) A formula including Legendre’s E ⁒ K + K ⁒ E K ⁒ K = 1 2 ⁒ Ο€ . Messenger of Math. 33, pp. 31–32.
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  • A. Erdélyi, W. Magnus, F. Oberhettinger, and F. G. Tricomi (1953b) Higher Transcendental Functions. Vol. II. McGraw-Hill Book Company, Inc., New York-Toronto-London.
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  • F. H. L. Essler, H. Frahm, A. R. Its, and V. E. Korepin (1996) Painlevé transcendent describes quantum correlation function of the X ⁒ X ⁒ Z antiferromagnet away from the free-fermion point. J. Phys. A 29 (17), pp. 5619–5626.
  • 25: 26.12 Plane Partitions
    β–ΊWe define the r × s × t box B ⁑ ( r , s , t ) as …Then the number of plane partitions in B ⁑ ( r , s , t ) is … β–ΊThe number of symmetric plane partitions in B ⁑ ( r , r , t ) is … β–ΊThe complement of Ο€ B ⁑ ( r , s , t ) is Ο€ c = { ( h , j , k ) | ( r h + 1 , s j + 1 , t k + 1 ) Ο€ } . … β–ΊThe number of descending plane partitions in B ⁑ ( r , r , r ) is …
    26: Bibliography U
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  • F. Ursell (1960) On Kelvin’s ship-wave pattern. J. Fluid Mech. 8 (3), pp. 418–431.
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  • F. Ursell (1972) Integrals with a large parameter. Several nearly coincident saddle-points. Proc. Cambridge Philos. Soc. 72, pp. 49–65.
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  • F. Ursell (1980) 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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  • F. Ursell (1984) 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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  • K. M. Urwin and F. M. Arscott (1970) Theory of the Whittaker-Hill equation. Proc. Roy. Soc. Edinburgh Sect. A 69, pp. 28–44.
  • 27: Bibliography Y
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  • Z. M. Yan (1992) 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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  • A. Yu. Yeremin, I. E. Kaporin, and M. K. Kerimov (1988) 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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  • J. M. Yohe (1979) Software for interval arithmetic: A reasonably portable package. ACM Trans. Math. Software 5 (1), pp. 50–63.
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  • T. Yoshida (1995) Computation of Kummer functions U ⁒ ( a , b , x ) for large argument x by using the Ο„ -method. Trans. Inform. Process. Soc. Japan 36 (10), pp. 2335–2342 (Japanese).
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  • A. P. Yutsis, I. B. Levinson, and V. V. Vanagas (1962) 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
    β–ΊIn the following formulas for the coefficients A k ⁑ ( ΞΆ ) , B k ⁑ ( ΞΆ ) , C k ⁑ ( ΞΆ ) , and D k ⁑ ( ΞΆ ) , u k , v k are the constants defined in §9.7(i), and U k ⁑ ( p ) , V k ⁑ ( p ) are the polynomials in p of degree 3 ⁒ k defined in §10.41(ii). … β–ΊNote: Another way of arranging the above formulas for the coefficients A k ⁑ ( ΞΆ ) , B k ⁑ ( ΞΆ ) , C k ⁑ ( ΞΆ ) , and D k ⁑ ( ΞΆ ) would be by analogy with (12.10.42) and (12.10.46). … β–ΊEach of the coefficients A k ⁑ ( ΞΆ ) , B k ⁑ ( ΞΆ ) , C k ⁑ ( ΞΆ ) , and D k ⁑ ( ΞΆ ) , k = 0 , 1 , 2 , , is real and infinitely differentiable on the interval < ΞΆ < . … β–ΊFor numerical tables of ΞΆ = ΞΆ ⁑ ( z ) , ( 4 ⁒ ΞΆ / ( 1 z 2 ) ) 1 4 and A k ⁑ ( ΞΆ ) , B k ⁑ ( ΞΆ ) , C k ⁑ ( ΞΆ ) , and D k ⁑ ( ΞΆ ) see Olver (1962, pp. 28–42). …
    29: 10.21 Zeros
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    §10.21(vi) McMahon’s Asymptotic Expansions for Large Zeros
    β–ΊWith a = ( t + 1 2 ⁒ Ξ½ 1 4 ) ⁒ Ο€ , the right-hand side is the asymptotic expansion of ρ Ξ½ ⁑ ( t ) for large t . … β–Ί
    §10.21(vii) Asymptotic Expansions for Large Order
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    §10.21(viii) Uniform Asymptotic Approximations for Large Order
    β–Ί B 0 ⁑ ( ΞΆ ) and C 0 ⁑ ( ΞΆ ) are defined by (10.20.11) and (10.20.12) with k = 0 . …
    30: Bibliography P
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  • R. B. Paris and A. D. Wood (1995) Stokes phenomenon demystified. Bull. Inst. Math. Appl. 31 (1-2), pp. 21–28.
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  • R. B. Paris (2004) 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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  • J. K. Patel and C. B. Read (1982) Handbook of the Normal Distribution. Statistics: Textbooks and Monographs, Vol. 40, Marcel Dekker Inc., New York.
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  • R. Piessens and M. Branders (1984) Algorithm 28. Algorithm for the computation of Bessel function integrals. J. Comput. Appl. Math. 11 (1), pp. 119–137.
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  • M. H. Protter and C. B. Morrey (1991) A First Course in Real Analysis. 2nd edition, Undergraduate Texts in Mathematics, Springer-Verlag, New York.