So let's try and tackle the first order derivative, $\partial_x(xp)=p+x\partial_x p$, let's look at the Fourier of the second term:
$F(x\partial_x p)=\int_{\mathbb R}x\partial_xpe^{-2\pi i xw}\,dx$
Notice that $\partial_we^{-2\pi i xw}=-2\pi ixe^{-2\pi i xw}$ so
$F(x\partial_x p)=\frac{i}{2\pi}\partial_wF(\partial_xp)=-w\partial_wF(p)$. By the way I may be out by some constants, but use the magic $2\pi=1$ formula and its all good.