Abstract

The inclusive cross sections, measured up to large values of effective mass ($\ensuremath{\equiv}\frac{{q}^{2}}{2\ensuremath{\nu}}$), are well fitted by $\frac{d\ensuremath{\sigma}}{{d}^{3}p}={B}_{x}\mathrm{exp}(\ensuremath{-}\frac{{\ensuremath{\alpha}}_{x}{p}^{2}}{2{m}_{x}})$. Values of ${B}_{x}$ and ${\ensuremath{\alpha}}_{x}$ are given for Be, C, Cu, and Ta at the incident proton energy of 600 MeV and for Ag, Ta, and Pt at 800 MeV. Extremely large $\frac{d}{p}$ and $\frac{t}{p}$ ratios and large $A$ and ${q}^{2}$ dependences of the relative cross sections are observed.

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