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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\in\mathbb{R} and t>0,

7.19.1 \mathsf{U}\left(x,t\right)=\frac{1}{\sqrt{4\pi t}}\int_{-\infty}^{\infty}\frac%
{e^{-(x-y)^{2}/(4t)}}{1+y^{2}}\,\mathrm{d}y,
7.19.2 \mathsf{V}\left(x,t\right)=\frac{1}{\sqrt{4\pi t}}\int_{-\infty}^{\infty}\frac%
{ye^{-(x-y)^{2}/(4t)}}{1+y^{2}}\,\mathrm{d}y.
7.19.4 H\left(a,u\right)=\frac{a}{\pi}\int_{-\infty}^{\infty}\frac{e^{-t^{2}}\,%
\mathrm{d}t}{(u-t)^{2}+a^{2}}=\frac{1}{a\sqrt{\pi}}\mathsf{U}\left(\frac{u}{a}%
,\frac{1}{4a^{2}}\right).

H\left(a,u\right) 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 \mathsf{U}\left(x,t\right), t=0.1, 2.5, 5, 10. Magnify
See accompanying text
Figure 7.19.2: Voigt function \mathsf{V}\left(x,t\right), t=0.1, 2.5, 5, 10. Magnify

§7.19(iii) Properties

7.19.5
\lim_{t\to 0}\mathsf{U}\left(x,t\right)=\frac{1}{1+x^{2}},
\lim_{t\to 0}\mathsf{V}\left(x,t\right)=\frac{x}{1+x^{2}}.
7.19.6
\mathsf{U}\left(-x,t\right)=\mathsf{U}\left(x,t\right),
\mathsf{V}\left(-x,t\right)=-\mathsf{V}\left(x,t\right).
7.19.7
0<\mathsf{U}\left(x,t\right)\leq 1,
-1\leq\mathsf{V}\left(x,t\right)\leq 1.

§7.19(iv) Other Integral Representations

7.19.10 \mathsf{U}\left(\frac{u}{a},\frac{1}{4a^{2}}\right)=a\int_{0}^{\infty}e^{-at-%
\frac{1}{4}t^{2}}\cos\left(ut\right)\,\mathrm{d}t,
7.19.11 \mathsf{V}\left(\frac{u}{a},\frac{1}{4a^{2}}\right)=a\int_{0}^{\infty}e^{-at-%
\frac{1}{4}t^{2}}\sin\left(ut\right)\,\mathrm{d}t.