Positive-energy on-shell delta function identity
= Positive-energy on-shell delta function identity
{title2=$\frac{\delta(\omega-E)}{E}=2\delta(E^2-\omega^2),\quad \omega>0$}
For $E>0$ and the positive-energy branch, the root Jacobian of the <Dirac delta function> gives this identity. In a <massless collinear parton approximation>, it produces $\delta(x-\xi)/(P\cdot q)$.