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11: 7.10 Derivatives
§7.10 Derivatives
7.10.1 d n + 1 erf z d z n + 1 = ( 1 ) n 2 π H n ( z ) e z 2 , n = 0 , 1 , 2 , .
7.10.2 w ( z ) = 2 z w ( z ) + ( 2 i / π ) ,
d g ( z ) d z = π z f ( z ) 1 .
12: 7.11 Relations to Other Functions
§7.11 Relations to Other Functions
Incomplete Gamma Functions and Generalized Exponential Integral
Confluent Hypergeometric Functions
7.11.6 C ( z ) + i S ( z ) = z M ( 1 2 , 3 2 , 1 2 π i z 2 ) = z e π i z 2 / 2 M ( 1 , 3 2 , 1 2 π i z 2 ) .
Generalized Hypergeometric Functions
13: 7.19 Voigt Functions
7.19.2 𝖵 ( x , t ) = 1 4 π t y e ( x y ) 2 / ( 4 t ) 1 + y 2 d y .
7.19.4 H ( a , u ) = a π e t 2 d t ( u t ) 2 + a 2 = 1 a π 𝖴 ( u a , 1 4 a 2 ) .
14: 19.14 Reduction of General Elliptic Integrals
§19.14 Reduction of General Elliptic Integrals
Legendre (1825–1832) showed that every elliptic integral can be expressed in terms of the three integrals in (19.1.2) supplemented by algebraic, logarithmic, and trigonometric functions. The classical method of reducing (19.2.3) to Legendre’s integrals is described in many places, especially Erdélyi et al. (1953b, §13.5), Abramowitz and Stegun (1964, Chapter 17), and Labahn and Mutrie (1997, §3). …A similar remark applies to the transformations given in Erdélyi et al. (1953b, §13.5) and to the choice among explicit reductions in the extensive table of Byrd and Friedman (1971), in which one limit of integration is assumed to be a branch point of the integrand at which the integral converges. …
15: 9.13 Generalized Airy Functions
Swanson and Headley (1967) define independent solutions A n ( z ) and B n ( z ) of (9.13.1) by … Their relations to the functions A n ( z ) and B n ( z ) are given by … When α is a positive integer the relation of these functions to W m ( t ) , W m ( t ) is as follows: … The A k ( z , p ) are related by … Further properties of these functions, and also of similar contour integrals containing an additional factor ( ln t ) q , q = 1 , 2 , , in the integrand, are derived in Reid (1972), Drazin and Reid (1981, Appendix), and Baldwin (1985). …
16: 13.18 Relations to Other Functions
§13.18 Relations to Other Functions
§13.18(i) Elementary Functions
§13.18(iv) Parabolic Cylinder Functions
§13.18(v) Orthogonal Polynomials
Laguerre Polynomials
17: 7.13 Zeros
§7.13(iii) Zeros of the Fresnel Integrals
As n the x n and y n corresponding to the zeros of C ( z ) satisfy … As n the x n and y n corresponding to the zeros of S ( z ) satisfy (7.13.5) with … In consequence of (7.5.5) and (7.5.10), zeros of ( z ) are related to zeros of erfc z . …
18: 1.8 Fourier Series
Here c n is related to a n and b n in (1.8.1), (1.8.2) by c n = 1 2 ( a n i b n ) , c n = 1 2 ( a n + i b n ) for n > 0 and c 0 = 1 2 a 0 . … As n (1.8.10) continues to apply if either a or b or both are infinite and/or f ( x ) has finitely many singularities in ( a , b ) , provided that the integral converges uniformly (§1.5(iv)) at a , b , and the singularities for all sufficiently large λ . … Then the series (1.8.1) converges to the sum … It follows from definition (1.14.1) that the integral in (1.8.14) is equal to 2 π ( f ) ( 2 π n ) . …
19: 13.6 Relations to Other Functions
§13.6 Relations to Other Functions
§13.6(iv) Parabolic Cylinder Functions
§13.6(v) Orthogonal Polynomials
Laguerre Polynomials
§13.6(vi) Generalized Hypergeometric Functions
20: 19.25 Relations to Other Functions
§19.25(ii) Bulirsch’s Integrals as Symmetric Integrals
§19.25(iv) Theta Functions
§19.25(vii) Hypergeometric Function