In the early eighties, L\'opez, Gonz\'alez-Arroyo and the present author proved that, if at a given $Q_0^2$ large enough for perturbative QCD to be valid, structure functions behave as a power of $x$ for $x\rightarrow 0$, then for all larger $Q^2$ one has $$F_2(x,Q^2)\simeq B_S[\alpha_s(Q^2)]^{ -d_+}x^{ -\lambda} +B_{ NS}[\alpha_s(Q^2)]^{ -D_{ 11}}x^{ 0.5},$$ $$F_G(x,Q^2)\simeq B_G[\alpha_s(Q^2)]^{ -d_+}x^{ -\lambda}$$ $$R(x,Q^2)=\frac{ r_0\alpha_s(Q^2)}{ \pi},$$ with $D_{ 11},\,d_+,\,B_G,\,r_0$ calculable in terms of $B_S,\,\lambda$. Moreover, it was suggested that the ``hard" part of the scattering cross section for real photons (Compton scattering) obeys a similar law, so that $$\sigma_{ \gamma p}\simeq B_{ \gamma p}s^{ \lambda}+A_{ \gamma p}\hat{ \sigma}^P,$$ with a value of $\lambda$ comparable to that in the expression for the structure functions, and where $\hat{ \sigma}^P\sim\log^2s$ is a universal, Pomeron-type cross section, and $A_{ \gamma p},\, B_{ \gamma p}$ are constants. In the present paper it is shown that the recent HERA measurements may be described by these formulas, with a chi-sqared/d.o.f. substantially less than unity, and with values of the parameters compatible with those of the old fits of the '80s. Moreover, further discussions are presented both on the low $Q^2$ limit, and the transition between Compton and deep inelastic scattering, in particular in connection with possible saturation of the coupling constant $\alpha_s(Q^2)$ at small $Q^2$; and on the ultra high energy limit, and how one might test the so-called BFKL conjecture, $$\lim_{ x\rightarrow 0\atop Q^2\rightarrow \infty}F_2(x,Q^2)\sim x^{ -c_0\alpha_s}.$$\hb With respect to the last we find some evidence against
Categories: hep-ph