Without loss of generality, we may assume that $y=0$.
$$
\widehat{\delta_x-\delta_0}(\xi)=e^{ix\cdot\xi}-1.
$$
Then
$$\begin{align}
\|\delta_x-\delta_0\|_{H^{-s}}^2&=\int_{\mathbb{R}^n}(1+|\xi|^2)^{-s}|e^{ix\cdot\xi}-1|^2\,d\xi\\
&=4\int_{\mathbb{R}^n}(1+|\xi|^2)^{-s}\sin^2\frac{x\cdot\xi}{2}\,d\xi\\
&=4\int_{\mathbb{R}^n}\Bigl(1+\frac{|\eta|^2}{|x|^2}\Bigr)^{-s}\sin^2\frac{x\cdot\eta}{2\,|x|}\,\frac{d\eta}{|x|^n}\\
&=4\,|x|^{2\alpha}\int_{\mathbb{R}^n}\bigl(|x|^2+|\xi|^2\bigr)^{-s}\sin^2\frac{x\cdot\eta}{2\,|x|}\,d\eta.
\end{align}$$
I leave to you to show that the last integral is bounded independently of $x$.