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41—46 of 46 matching pages

41: Bibliography C
  • B. C. Carlson (2006b) Table of integrals of squared Jacobian elliptic functions and reductions of related hypergeometric R -functions. Math. Comp. 75 (255), pp. 1309–1318.
  • R. C. Y. Chin and G. W. Hedstrom (1978) A dispersion analysis for difference schemes: Tables of generalized Airy functions. Math. Comp. 32 (144), pp. 1163–1170.
  • W. J. Cody (1991) Performance evaluation of programs related to the real gamma function. ACM Trans. Math. Software 17 (1), pp. 46–54.
  • E. D. Constantinides and R. J. Marhefka (1993) Efficient and accurate computation of the incomplete Airy functions. Radio Science 28 (4), pp. 441–457.
  • R. M. Corless, D. J. Jeffrey, and H. Rasmussen (1992) Numerical evaluation of Airy functions with complex arguments. J. Comput. Phys. 99 (1), pp. 106–114.
  • 42: 12.14 The Function W ( a , x )
    §12.14 The Function W ( a , x )
    §12.14(vii) Relations to Other Functions
    Bessel Functions
    Confluent Hypergeometric Functions
    Airy-type Uniform Expansions
    43: 36.7 Zeros
    This is the Airy function Ai 9.2). … Close to the y -axis the approximate location of these zeros is given by … Deep inside the bifurcation set, that is, inside the three-cusped astroid (36.4.10) and close to the part of the z -axis that is far from the origin, the zero contours form an array of rings close to the planes …Outside the bifurcation set (36.4.10), each rib is flanked by a series of zero lines in the form of curly “antelope horns” related to the “outside” zeros (36.7.2) of the cusp canonical integral. There are also three sets of zero lines in the plane z = 0 related by 2 π / 3 rotation; these are zeros of (36.2.20), whose asymptotic form in polar coordinates ( x = r cos θ , y = r sin θ ) is given by …
    44: 12.10 Uniform Asymptotic Expansions for Large Parameter
    The turning points can be included if expansions in terms of Airy functions are used instead of elementary functions2.8(iii)). …
    §12.10(vii) Negative a , 2 a < x < . Expansions in Terms of Airy Functions
    Modified Expansions
    §12.10(viii) Negative a , < x < 2 a . Expansions in Terms of Airy Functions
    45: Bibliography H
  • P. I. Hadži (1978) Sums with cylindrical functions that reduce to the probability function and to related functions. Bul. Akad. Shtiintse RSS Moldoven. 1978 (3), pp. 80–84, 95 (Russian).
  • G. H. Hardy and E. M. Wright (1979) An Introduction to the Theory of Numbers. 5th edition, The Clarendon Press Oxford University Press, New York-Oxford.
  • V. B. Headley and V. K. Barwell (1975) On the distribution of the zeros of generalized Airy functions. Math. Comp. 29 (131), pp. 863–877.
  • G. J. Heckman (1991) An elementary approach to the hypergeometric shift operators of Opdam. Invent. Math. 103 (2), pp. 341–350.
  • F. B. Hildebrand (1974) Introduction to Numerical Analysis. 2nd edition, McGraw-Hill Book Co., New York.
  • 46: 10.21 Zeros
    The functions ρ ν ( t ) and σ ν ( t ) are related to the inverses of the phase functions θ ν ( x ) and ϕ ν ( x ) defined in §10.18(i): if ν 0 , then … Let 𝒞 ν ( x ) , ρ ν ( t ) , and σ ν ( t ) be defined as in §10.21(ii) and M ( x ) , θ ( x ) , N ( x ) , and ϕ ( x ) denote the modulus and phase functions for the Airy functions and their derivatives as in §9.8. … Here a m and a m denote respectively the zeros of the Airy function Ai ( z ) and its derivative Ai ( z ) ; see §9.9. … Corresponding uniform approximations for y ν , m , Y ν ( y ν , m ) , y ν , m , and Y ν ( y ν , m ) , are obtained from (10.21.41)–(10.21.44) by changing the symbols j , J , Ai , Ai , a m , and a m to y , Y , Bi , Bi , b m , and b m , respectively. …
    §10.21(xiv) ν -Zeros