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31: 7.12 Asymptotic Expansions
§7.12(i) Complementary Error Function
erfc z e z 2 π m = 0 ( 1 ) m ( 1 2 ) m z 2 m + 1 ,
erfc ( z ) 2 e z 2 π m = 0 ( 1 ) m ( 1 2 ) m z 2 m + 1 ,
For these and other error bounds see Olver (1997b, pp. 109–112), with α = 1 2 and z replaced by z 2 ; compare (7.11.2). … (Note that some of these re-expansions themselves involve the complementary error function.) …
32: 13.6 Relations to Other Functions
§13.6(ii) Incomplete Gamma Functions
Special cases are the error functions
13.6.7 M ( 1 2 , 3 2 , z 2 ) = π 2 z erf ( z ) ,
33: 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 .
7.19.3 𝖴 ( x , t ) + i 𝖵 ( x , t ) = π 4 t e z 2 erfc z , z = ( 1 i x ) / ( 2 t ) .
34: 2.11 Remainder Terms; Stokes Phenomenon
Here erfc is the complementary error function7.2(i)), and … Hence from §7.12(i) erfc ( 1 2 ρ c ( θ ) ) is of the same exponentially-small order of magnitude as the contribution from the other terms in (2.11.15) when ρ is large. On the other hand, when π + δ θ 3 π δ , c ( θ ) is in the left half-plane and erfc ( 1 2 ρ c ( θ ) ) differs from 2 by an exponentially-small quantity. In the transition through θ = π , erfc ( 1 2 ρ c ( θ ) ) changes very rapidly, but smoothly, from one form to the other; compare the graph of its modulus in Figure 2.11.1 in the case ρ = 100 .
See accompanying text
Figure 2.11.1: Graph of | erfc ( 50 c ( θ ) ) | . Magnify
35: 32.10 Special Function Solutions
32.10.22 w ( z ) = { 2 exp ( z 2 ) π ( C i erfc ( i z ) ) , ε = 1 , 2 exp ( z 2 ) π ( C erfc ( z ) ) , ε = 1 ,
where C is an arbitrary constant and erfc is the complementary error function7.2(i)). …
36: 8.18 Asymptotic Expansions of I x ( a , b )
8.18.9 I x ( a , b ) 1 2 erfc ( η b / 2 ) + 1 2 π ( a + b ) ( x x 0 ) a ( 1 x 1 x 0 ) b k = 0 ( 1 ) k c k ( η ) ( a + b ) k ,
For erfc see §7.2(i). …
37: 3.5 Quadrature
Example
where erfc z is the complementary error function, and from (7.12.1) it follows that
Table 3.5.20: Composite trapezoidal rule for the integral (3.5.45) with λ = 10 .
h erfc λ n
38: 12.11 Zeros
When a = 1 2 these zeros are the same as the zeros of the complementary error function erfc ( z / 2 ) ; compare (12.7.5). …
39: Nico M. Temme
40: 8.11 Asymptotic Approximations and Expansions