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31: Brian D. Sleeman
Sleeman published numerous papers in applied analysis, multiparameter spectral theory, direct and inverse scattering theory, and mathematical medicine. …
32: 19.37 Tables
Tabulated for arcsin k = 0 ( 1 ) 90 to 6D by Byrd and Friedman (1971) and to 15D by Abramowitz and Stegun (1964, Chapter 17). … Tabulated for arcsin k = 0 ( 1 ) 90 to 6D by Byrd and Friedman (1971) and to 15D by Abramowitz and Stegun (1964, Chapter 17). … Tabulated for ϕ = 0 ( 5 ) 90 , arcsin k = 0 ( 1 ) 90 to 6D by Byrd and Friedman (1971), for ϕ = 0 ( 5 ) 90 , arcsin k = 0 ( 2 ) 90 and 5 ( 10 ) 85 to 8D by Abramowitz and Stegun (1964, Chapter 17), and for ϕ = 0 ( 10 ) 90 , arcsin k = 0 ( 5 ) 90 to 9D by Zhang and Jin (1996, pp. 674–675). … Tabulated (with different notation) for ϕ = 0 ( 15 ) 90 , α 2 = 0 ( .1 ) 1 , arcsin k = 0 ( 15 ) 90 to 5D by Abramowitz and Stegun (1964, Chapter 17), and for ϕ = 0 ( 15 ) 90 , α 2 = 0 ( .1 ) 1 , arcsin k = 0 ( 15 ) 90 to 7D by Zhang and Jin (1996, pp. 676–677). …
33: 35.2 Laplace Transform
Inversion Formula
34: 19.17 Graphics
35: 24.5 Recurrence Relations
§24.5(iii) Inversion Formulas
36: 19.2 Definitions
In (19.2.18)–(19.2.22) the inverse trigonometric and hyperbolic functions assume their principal values (§§4.23(ii) and 4.37(ii)). When x and y are positive, R C ( x , y ) is an inverse circular function if x < y and an inverse hyperbolic function (or logarithm) if x > y :
19.2.18 R C ( x , y ) = 1 y x arctan y x x = 1 y x arccos x / y , 0 x < y ,
19.2.19 R C ( x , y ) = 1 x y arctanh x y x = 1 x y ln x + x y y , 0 < y < x .
19.2.20 R C ( x , y ) = x x y R C ( x y , y ) = 1 x y arctanh x x y = 1 x y ln x + x y y , y < 0 x .
37: 1.1 Special Notation
x , y real variables.
𝐀 1 inverse of the square matrix 𝐀
38: 15.14 Integrals
Inverse Laplace transforms of hypergeometric functions are given in Erdélyi et al. (1954a, §5.19), Oberhettinger and Badii (1973, §2.18), and Prudnikov et al. (1992b, §3.35). …Inverse Mellin transforms are given in Erdélyi et al. (1954a, §7.5). …
39: 19.12 Asymptotic Approximations
19.12.6 R C ( x , y ) = π 2 y x y ( 1 + O ( x y ) ) , x / y 0 ,
19.12.7 R C ( x , y ) = 1 2 x ( ( 1 + y 2 x ) ln ( 4 x y ) y 2 x ) ( 1 + O ( y 2 / x 2 ) ) , y / x 0 .
40: 36.13 Kelvin’s Ship-Wave Pattern
θ + ( ϕ ) = 1 2 ( arcsin ( 3 sin ϕ ) ϕ ) ,
θ ( ϕ ) = 1 2 ( π ϕ arcsin ( 3 sin ϕ ) ) .
36.13.5 | ϕ | = ϕ c = arcsin ( 1 3 ) = 19 .47122 .