Measurements of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>A</mml:mi></mml:math>Dependence of Deep-Inelastic Electron Scattering from Nuclei

R. G. Arnold(American University), P. Bosted(American University), C. C. Chang(American University), J. Gómez(American University), A. T. Katramatou(American University), G. G. Petratos(American University), A. A. Rahbar(American University), S. E. Rock(American University), A. F. Sill(American University), Z. M. Szalata(American University), A. Bodek(University of Rochester), N. Giokaris(American University), D. J. Sherden(Stanford Synchrotron Radiation Lightsource), B. A. Mecking(University of Bonn), R.M. Lombard(CEA Paris-Saclay)
Physical Review Letters
February 27, 1984
Cited by 418

Abstract

The deep-inelastic electron-scattering cross sections per nucleon ${\ensuremath{\sigma}}_{A}$ for D, He, Be, C, A1, Ca, Fe, Ag, and Au were measured in the kinematic range $0.09&lt;~x&lt;~0.9$ and $2&lt;~{Q}^{2}&lt;~15$ ${(\mathrm{G}\mathrm{e}\mathrm{V}/\mathit{c})}^{2}$ with use of electrons with energies ranging from 8 to 24.5 GeV. The ratio $\frac{{\ensuremath{\sigma}}_{A}}{{\ensuremath{\sigma}}_{\mathrm{D}}}$ is consistent with unity in the range $0.1&lt;x&lt;0.3$. For $0.3&lt;x&lt;0.8$, the ratio decreases logarithmically with atomic weight $A$, or linearly with average nuclear density. No ${Q}^{2}$ dependence in the ratio was observed over the kinematic range of the data.


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