The following integral
$$\frac{2\pi}{ir}\int_{0}^{\infty}ke^{-i\omega_kt}(e^{ikr}-e^{-ikr})dk$$
arises in finding the probability amplitude: $\langle x|e^{-i\hat{H}t}|x=0\rangle$. Here $\vec{x} = r\hat{z}$; $k$ is the angular wave number; $\omega_k = \sqrt{m^2+k^2}$, and $m$ is the mass of the particle
Kindly point me to some web resources or some textbook where I could learn to solve/decipher this integral; or why it can or cannot be solved and its consequences.
Hints: