You are mistaken. The integral along the circular arc emphatically does not vanish. You can see this by writing it out:
$$i R \int_0^{\pi} d\theta \, e^{i \theta} \, e^{i a R e^{i \theta}} \frac{1-e^{-b R^2 e^{i 2 \theta}}}{R^2 e^{i 2 \theta}} $$
The magnitude of this integral is bounded by
$$\frac1{R} \int_0^{\pi} d\theta \, e^{-a R \sin{\theta}} \left |1-e^{-b R^2 \cos{2 \theta}} \right |$$
Note that, while $\sin{\theta} \gt 0$ over the region of integration, $\cos{2 \theta}$ is not. Rather, when $b \gt 0$, $\cos{2 \theta} \lt 0$ when $\theta \in [\pi/4,3 \pi/4]$. Within this region, the gaussian term rapidly overwhelms the exponential term and the integral blows up. We thus learn nothing from bounding the integral around the circular arc except that you cannot make a statement about the Fourier transform integral as you have done.