7 Error Functions, Dawson’s and Fresnel IntegralsProperties

§7.19 Voigt Functions

Contents
  1. §7.19(i) Definitions
  2. §7.19(ii) Graphics
  3. §7.19(iii) Properties
  4. §7.19(iv) Other Integral Representations

§7.19(i) Definitions

For x∈ℝ and t>0,

7.19.1 𝖴⁡(x,t)=14⁢π⁢t⁢∫−∞∞e−(x−y)2/(4⁢t)1+y2⁢dy,
7.19.2 𝖵⁡(x,t)=14⁢π⁢t⁢∫−∞∞y⁢e−(x−y)2/(4⁢t)1+y2⁢dy.
7.19.4 H⁡(a,u)=aπ⁢∫−∞∞e−t2⁢dt(u−t)2+a2=1a⁢π⁢𝖴⁡(ua,14⁢a2).

H⁡(a,u) is sometimes called the line broadening function; see, for example, Finn and Mugglestone (1965).

§7.19(ii) Graphics

See accompanying text
Figure 7.19.1: Voigt function 𝖴⁡(x,t), t=0.1, 2.5, 5, 10. Magnify
See accompanying text
Figure 7.19.2: Voigt function 𝖵⁡(x,t), t=0.1, 2.5, 5, 10. Magnify

§7.19(iii) Properties

7.19.5 limt→0𝖴⁡(x,t) =11+x2,
limt→0𝖵⁡(x,t) =x1+x2.
7.19.6 𝖴⁡(−x,t) =𝖴⁡(x,t),
𝖵⁡(−x,t) =−𝖵⁡(x,t).
7.19.7 0 <𝖴⁡(x,t)≤1,
−1 ≤𝖵⁡(x,t)≤1.
7.19.8 𝖵⁡(x,t) =x⁢𝖴⁡(x,t)+2⁢t⁢∂𝖴⁡(x,t)∂x,
7.19.9 𝖴⁡(x,t) =1−x⁢𝖵⁡(x,t)−2⁢t⁢∂𝖵⁡(x,t)∂x.

§7.19(iv) Other Integral Representations

7.19.10 𝖴⁡(ua,14⁢a2)=a⁢∫0∞e−a⁢t−14⁢t2⁢cos⁡(u⁢t)⁢dt,
7.19.11 𝖵⁡(ua,14⁢a2)=a⁢∫0∞e−a⁢t−14⁢t2⁢sin⁡(u⁢t)⁢dt.