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41: 36.12 Uniform Approximation of Integrals
The function g has a smooth amplitude. …
36.12.4 f ( u ( t , 𝐲 ) ; 𝐲 ) = A ( 𝐲 ) + Φ K ( t ; 𝐱 ( 𝐲 ) ) ,
with the K + 1 functions A ( 𝐲 ) and 𝐱 ( 𝐲 ) determined by correspondence of the K + 1 critical points of f and Φ K . …
36.12.5 f ( u j ( 𝐲 ) ; 𝐲 ) = A ( 𝐲 ) + Φ K ( t j ( 𝐱 ( 𝐲 ) ) ; 𝐱 ( 𝐲 ) ) ,
36.12.6 A ( 𝐲 ) = f ( u ( 0 , 𝐲 ) ; 𝐲 ) ,
42: 13.2 Definitions and Basic Properties
M ( a , b , z ) is entire in z and a , and is a meromorphic function of b . …
13.2.35 𝒲 { 𝐌 ( a , b , z ) , e z U ( b a , b , e ± π i z ) } = e b π i z b e z / Γ ( b a ) ,
43: 12.20 Approximations
Luke (1969b, pp. 25 and 35) gives Chebyshev-series expansions for the confluent hypergeometric functions U ( a , b , x ) and M ( a , b , x ) 13.2(i)) whose regions of validity include intervals with endpoints x = and x = 0 , respectively. …
44: Bibliography L
  • A. Laforgia and M. E. Muldoon (1988) Monotonicity properties of zeros of generalized Airy functions. Z. Angew. Math. Phys. 39 (2), pp. 267–271.
  • A. Laforgia (1984) Further inequalities for the gamma function. Math. Comp. 42 (166), pp. 597–600.
  • A. Laforgia (1986) Inequalities for Bessel functions. J. Comput. Appl. Math. 15 (1), pp. 75–81.
  • A. Laforgia (1991) Bounds for modified Bessel functions. J. Comput. Appl. Math. 34 (3), pp. 263–267.
  • L. Lorch and P. Szegő (1964) Monotonicity of the differences of zeros of Bessel functions as a function of order. Proc. Amer. Math. Soc. 15 (1), pp. 91–96.
  • 45: 15.17 Mathematical Applications
    For harmonic analysis it is more natural to represent hypergeometric functions as a Jacobi function15.9(ii)). …Harmonic analysis can be developed for the Jacobi transform either as a generalization of the Fourier-cosine transform (§1.14(ii)) or as a specialization of a group Fourier transform. …
    46: 12.2 Differential Equations
    Standard solutions are U ( a , ± z ) , V ( a , ± z ) , U ¯ ( a , ± x ) (not complex conjugate), U ( a , ± i z ) for (12.2.2); W ( a , ± x ) for (12.2.3); D ν ( ± z ) for (12.2.4), where
    12.2.5 D ν ( z ) = U ( 1 2 ν , z ) .
    All solutions are entire functions of z and entire functions of a or ν . …
    §12.2(vi) Solution U ¯ ( a , x ) ; Modulus and Phase Functions
    When z ( = x ) is real the solution U ¯ ( a , x ) is defined by …
    47: 1.4 Calculus of One Variable
    A function f ( x ) is continuous on the right (or from above) at x = c if … A more general concept of integrability of a function on a bounded or unbounded interval is Lebesgue integrability, which allows discussion of functions which may not be well defined everywhere (especially on sets of measure zero) for x . … A function f ( x ) is square-integrable if … This definition also applies when f ( x ) is a complex function of the real variable x . … A function f ( x ) is convex on ( a , b ) if …
    48: 13.6 Relations to Other Functions
    When a b is an integer or a is a positive integer the Kummer functions can be expressed as incomplete gamma functions (or generalized exponential integrals). … When b = 2 a the Kummer functions can be expressed as modified Bessel functions. …
    13.6.11_1 M ( ν + 1 2 , 2 ν + 1 + n , 2 z ) = Γ ( ν ) e z ( z / 2 ) ν k = 0 n ( n ) k ( 2 ν ) k ( ν + k ) ( 2 ν + 1 + n ) k k ! I ν + k ( z ) ,
    49: 36.13 Kelvin’s Ship-Wave Pattern
    36.13.1 z ( ϕ , ρ ) = π / 2 π / 2 cos ( ρ cos ( θ + ϕ ) cos 2 θ ) d θ ,
    The wake is a caustic of the “rays” defined by the dispersion relation (“Hamiltonian”) giving the frequency ω as a function of wavevector 𝐤 : …
    36.13.8 z ( ρ , ϕ ) = 2 π ( ρ 1 / 3 u ( ϕ ) cos ( ρ f ~ ( ϕ ) ) Ai ( ρ 2 / 3 Δ ( ϕ ) ) ( 1 + O ( 1 / ρ ) ) + ρ 2 / 3 v ( ϕ ) sin ( ρ f ~ ( ϕ ) ) Ai ( ρ 2 / 3 Δ ( ϕ ) ) ( 1 + O ( 1 / ρ ) ) ) , ρ .
    See accompanying text
    Figure 36.13.1: Kelvin’s ship wave pattern, computed from the uniform asymptotic approximation (36.13.8), as a function of x = ρ cos ϕ , y = ρ sin ϕ . Magnify
    50: 15.2 Definitions and Analytical Properties
    The hypergeometric function F ( a , b ; c ; z ) is defined by the Gauss seriesThe principal branch of 𝐅 ( a , b ; c ; z ) is an entire function of a , b , and c . …As a multivalued function of z , 𝐅 ( a , b ; c ; z ) is analytic everywhere except for possible branch points at z = 0 , 1 , and . The same properties hold for F ( a , b ; c ; z ) , except that as a function of c , F ( a , b ; c ; z ) in general has poles at c = 0 , 1 , 2 , . … For example, when a = m , m = 0 , 1 , 2 , , and c 0 , 1 , 2 , , F ( a , b ; c ; z ) is a polynomial: …