Abstract

We examine the implication of the unitarity bounds for the differential cross section to the break structure of the forward peak of elastic pp and p\ifmmode\bar\else\textasciimacron\fi{}p scattering observed at the squared momentum transfer \ensuremath{\Vert}t\ensuremath{\Vert}=0.1--0.15 (GeV/c${)}^{2}$ at high energies. The break is suggested to occur at around 8.8/${\mathit{R}}_{0}^{2}$\ensuremath{\Vert}t\ensuremath{\Vert}14.7/${\mathit{R}}_{0}^{2}$, ${\mathit{R}}_{0}$ being the interaction radius given in terms of ${\mathrm{\ensuremath{\sigma}}}_{\mathit{t}}^{2}$/${\mathrm{\ensuremath{\sigma}}}_{\mathrm{el}}$. This fits well with the experimental data of pp scattering in the energy region \ensuremath{\surd}s =10--60 GeV and p\ifmmode\bar\else\textasciimacron\fi{}p in 10--546 GeV. Scaling with the variable t${\mathrm{\ensuremath{\sigma}}}_{\mathit{t}}^{2}$/${\mathrm{\ensuremath{\sigma}}}_{\mathrm{el}}$ is discussed.

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