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11: 7.14 Integrals
7.14.1 0 e 2 i a t erfc ( b t ) d t = 1 a π F ( a b ) + i 2 a ( 1 e ( a / b ) 2 ) , a , | ph b | < 1 4 π .
12: 8.11 Asymptotic Approximations and Expansions
8.11.11 γ ( 1 a , x ) = x a 1 ( cos ( π a ) + sin ( π a ) π ( 2 π F ( y ) + 2 3 2 π a ( 1 y 2 ) ) e y 2 + O ( a 1 ) ) ,
For Dawson’s integral F ( y ) see §7.2(ii). …
13: 8.12 Uniform Asymptotic Expansions for Large Parameter
8.12.6 z a γ ( a , z ) = cos ( π a ) 2 sin ( π a ) ( e 1 2 a η 2 π F ( η a / 2 ) + T ( a , η ) ) ,
where F ( x ) is Dawson’s integral; see §7.2(ii). …
14: 7.7 Integral Representations
§7.7(i) Error Functions and Dawson’s Integral
7.7.3 0 e a t 2 + 2 i z t d t = 1 2 π a e z 2 / a + i a F ( z a ) , a > 0 .
15: 12.7 Relations to Other Functions
§12.7(ii) Error Functions, Dawson’s Integral, and Probability Function
16: 7 Error Functions, Dawson’s and Fresnel Integrals
Chapter 7 Error Functions, Dawson’s and Fresnel Integrals
17: 7.21 Physical Applications
Efficient algorithms for computing the Faddeeva (or Faddeyeva) function are discussed in Wells (1999), a paper frequently cited in the astrophysics literature. … Dawson’s integral appears in de-convolving even more complex motional effects; see Pratt (2007). …
18: 7.22 Methods of Computation
§7.22(i) Main Functions
19: Nico M. Temme
20: Bibliography J
  • A. J. E. M. Janssen (2021) Bounds on Dawson’s integral occurring in the analysis of a line distribution network for electric vehicles. Eurandom Preprint Series Technical Report 14, Eurandom, Eindhoven, The Netherlands.