 Physical momentum support of a deep-inelastic hadronic tensor

For an absorbed spacelike photon, use $q^2=-Q^2<0$, $\nu =P\cdot q>0$, $x=Q^2/(2\nu )$ and the physical momentum delta function ${\delta }^{(4)}(P+q-p_X)$. The displayed invariant final mass is compatible with deep inelastic scattering for $0<x<1$. Using $P-q$ with the same positive-$x$ definition instead gives $M^2-Q^2(1+1/x)$, which becomes negative in the Bjorken scaling limit and has no physical hadronic spectral support. Reversing the photon convention requires reversing the associated scalar-product and scaling-variable conventions too.