TY - JOUR
T1 - Proton total reaction cross sections for 22 isotopes of Ti, Fe, Ni, Cu, Zn, Zr, and Sn at 14.5 MeV
AU - Dicello, J. F.
AU - Igo, G. J.
AU - Roush, M. L.
PY - 1967
Y1 - 1967
N2 - Total proton reaction cross sections have been measured at 14.5 MeV for 22 separated isotope targets to an accuracy of 2% for Ti, Fe, Ni, Cu, Zn, and Zr isotopes and 4% for the Sn isotopes. A beam-attenuation technique employing a solid-state counter to detect elastically scattered protons at forward angles has been used. Use of the solid-state detector reduces the corrections due to inelastic processes to a negligible level. The total reaction cross sections for the Fe, Ni, Zn, and Zr isotopes increase more rapidly with increasing N than optical-model calculations based on 14.5-MeV elastic-scattering and polarization data predict. The measured values for Fe, Ni, Cu, Zn, and Zr isotopes were generally smaller than the optical-model predictions; the measured Sn values, however, were larger. The dip in R near Ni, previously observed using elemental targets in a number of experiments, is reproduced by suitable averaging of the isotope reaction cross sections. The dip is shown to arise from a combination of a sharply rising R with increasing N (for constant Z) and the relatively small average value of N for Ni due to shell closure.
AB - Total proton reaction cross sections have been measured at 14.5 MeV for 22 separated isotope targets to an accuracy of 2% for Ti, Fe, Ni, Cu, Zn, and Zr isotopes and 4% for the Sn isotopes. A beam-attenuation technique employing a solid-state counter to detect elastically scattered protons at forward angles has been used. Use of the solid-state detector reduces the corrections due to inelastic processes to a negligible level. The total reaction cross sections for the Fe, Ni, Zn, and Zr isotopes increase more rapidly with increasing N than optical-model calculations based on 14.5-MeV elastic-scattering and polarization data predict. The measured values for Fe, Ni, Cu, Zn, and Zr isotopes were generally smaller than the optical-model predictions; the measured Sn values, however, were larger. The dip in R near Ni, previously observed using elemental targets in a number of experiments, is reproduced by suitable averaging of the isotope reaction cross sections. The dip is shown to arise from a combination of a sharply rising R with increasing N (for constant Z) and the relatively small average value of N for Ni due to shell closure.
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U2 - 10.1103/PhysRev.157.1001
DO - 10.1103/PhysRev.157.1001
M3 - Article
AN - SCOPUS:0001536232
SN - 0031-899X
VL - 157
SP - 1001
EP - 1015
JO - Physical Review
JF - Physical Review
IS - 4
ER -