Nucleus-nucleus total cross sections for light nuclei at 1.55 and 2.89 GeV/<i>c</i>per nucleon

J. A. Jaros(University of California, Berkeley), A. Wagner(University of California, Berkeley), L. W. Anderson(University of California, Berkeley), O. Chamberlain(Lawrence Berkeley National Laboratory), R. Fuzesy(University of California, Berkeley), Jeffrey M. Gallup(Lawrence Berkeley National Laboratory), W. Gorn(University of California, Berkeley), L. S. Schroeder(Lawrence Berkeley National Laboratory), S. Shannon(University of California, Berkeley), G. Shapiro(Lawrence Berkeley National Laboratory), H. Steiner(University of California, Berkeley)
Physical Review C
November 1, 1978
Cited by 154

Abstract

We have measured total cross sections for protons, dueterons, $\ensuremath{\alpha}$ particles, and $^{12}\mathrm{C}$ on hydrogen, deuterium, helium, and carbon targets at 1.55 and 2.89 GeV/c nucleon using the "good geometry" transmission method. In addition, we measured the inelastic cross sections and elastic slope parameters for reactions initiated by deuterons, $\ensuremath{\alpha}$ particles, and $^{12}\mathrm{C}$. Our results are in good agreement with Glauber theory predictions, but the factorization relation ${\ensuremath{\sigma}}_{T}(\mathrm{AA})=\frac{{[{\ensuremath{\sigma}}_{T}(\mathrm{AB})]}^{2}}{{\ensuremath{\sigma}}_{T}(\mathrm{BB})}$ is not a good guide. We find ${\ensuremath{\sigma}}_{T}\ensuremath{\simeq}144{({{A}_{T}}^{\frac{1}{3}}\ensuremath{-}{{A}_{p}}^{\frac{1}{3}}\ensuremath{-}1.48)}^{2}$ mb and ${\ensuremath{\sigma}}_{\mathrm{IN}}\ensuremath{\simeq}78{({{A}_{T}}^{\frac{1}{3}}+{{A}_{p}}^{\frac{1}{3}}\ensuremath{-}1.25)}^{2}$ mb, where ${A}_{T}({A}_{p})$ is the atomic mass number of the target (projectile).NUCLEAR REACTIONS $^{12}\mathrm{C}(^{12}\mathrm{C}, X)$, ($\ensuremath{\alpha}, X$), ($d, X$), ($p, X$), $E=0.87 \mathrm{and} 2.10$ GeV/nucleon; measured total cross section, total inelastic cross section, and slope parameter of elastic scattering.


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