Technically speaking, there are two spikes, since $\sin \omega x = \frac 1 {2i} \left ( e^{i\omega x}-e^{-i \omega x}\right)$, and thus there 2 frequencies ($\omega$ and $-\omega$).
Also, technically, those spikes are really Dirac delta distributions.
Finally, if you think you're seeing some "area" instead of pure spikes, I'm guessing you are looking at a tool that discretized the $\sin$ and computed its Discrete Fourier Transform (so not the "integral" Fourier transform). That discretization has an effect of transforming the true delta into a finite spike with "some area" underneath.
Finally, if you reduce the discretization step of your $\sin$, then you'll start seeing the bump with an area look more and more like a spike. In the limit, this would become a true Dirac delta.