While evaluating the details of this paper by Taylor et al. I'm stuck at the following integral. In need to evaluate the following:
Regard $x$ as spatial x-coordinate & $t$ as time.
$I(x) = \int_{0}^{\infty} \{ \frac{cos(kx)-cos(k_0x)}{k^2-k_0^2}\}dk$ where $k_0\in (0,\infty)$ is some given fixed value and $x>0$. By tallying results of the paper & my calculations one can conclude that this must result in $Csin(k_0x)$ where $C$ is some constant.
Let $I(x) = I_1(x) -I_2(x)$ where $I_1(x) = \int_{0}^{\infty}\{\frac{cos(kx)}{k^2-k_0^2}\}dk$ and $I_2(x) = \int_{0}^{\infty}\{\frac{cos(k_0x)}{k^2-k_0^2}\}dk$.
Using complex analysis & some algebra
$I_1(x) = \frac{isin(k_0x)}{2k_0}\{\int_{-\infty}^{\infty}\frac{exp(ik)}{k}dk\}$
while
$ I_2(x) = \frac{cos(k_0x)}{2}\{\int_{-\infty}^{\infty}\frac{1}{k^2-k_0^2}dk\}$
Expanding the integrand of $I_2$ as an expanded partial fraction, one gets $I_2(x)=0.$
By Cauchy integral around a indented contour & applying Jordan's lemma(See Complex Variables and Applications,Churchill & Brown, 7th ed, Chap 7, Pgs 267-270 )
we find $\int_{-\infty}^{\infty}\frac{exp(ik)}{k}dk = i\pi$.
Thus $I(x)= \frac{-\pi sin(k_0x)}{2k_0}$