Let $\displaystyle \langle \psi_k,\phi\rangle = \int_{-\infty}^\infty \sin(kx)\phi(x)\,\mathrm{d}x,\ \phi \in \mathcal{C}_c^\infty(\Omega),\Omega\subset \mathbb{R}$ open. That means $\phi$ is a testfunction.
I want to compute
$\displaystyle \lim_{k\to \infty}\langle \psi_k,\phi\rangle$ and also $\displaystyle \lim_{k\to \infty}\langle \psi^2_k,\phi\rangle$
I know that for the fouriertransform $\mathcal{F}$ as a unitary operator it holds true that
$\langle \mathcal{F}\psi_k,\phi\rangle = \langle \psi_k,\mathcal{F}^{-1}\phi\rangle$
Using this I compute the inverse fourier transform of $\sin(kx)$ which yields
$\displaystyle i\sqrt{\frac{\pi}{2}}\delta(k+x)-i\sqrt{\frac{\pi}{2}}\delta(k-x)$
then I get
$\displaystyle \lim_{k\to\infty}\int_{-\infty}^{\infty}i\sqrt{\frac{\pi}{2}}\mathcal{F}^{-1}\phi(x) -i\sqrt{\frac{\pi}{2}}\mathcal{F}^{-1}\phi(-x)\,\mathrm{d}x$
which does not really help. Although I could solve the first (non-squared) one by using integration by parts (limit is then zero), I could not solve the squared version of it by using this technique, so I tried another strategy, which is the one I showed above.
Hint: $$ \sin^2(k\,x)=\frac{1-\cos(2\,k\,x)}{2}. $$