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- W152152693 abstract "A complete set of analyzing powers (AP's), ${mathit{iT}}_{11}$, ${mathit{T}}_{20}$, ${mathit{T}}_{21}$, and ${mathit{T}}_{22}$, for 50 MeV $^{12}mathrm{C}$${(}^{6}$Liensuremath{rightarrow}${,}^{6}$Li) elastic scattering and inelastic scattering to the $^{12}mathrm{C}$(${2}^{+}$, 4.44 MeV), $^{12}mathrm{C}$(${0}^{+}$, 7.65 MeV), and $^{12}mathrm{C}$(${3}^{mathrm{ensuremath{-}}}$, 9.64 MeV) states over the center-of-mass (c.m.) angular range 10ifmmode^circelsetextdegreefi{}--115ifmmode^circelsetextdegreefi{} is reported. In addition, cross sections for the excited states ${3}^{+}$(2.18 MeV), ${2}^{+}$(4.31 MeV), and ${1}^{+}$(5.65 MeV) of $^{6}mathrm{Li}$ were measured by using the inverse-kinematics reaction $^{6}mathrm{Li}$${(}^{12}$C${,}^{12}$C) at 100 MeV. A combined analysis of the new 50 MeV data and previous 30 MeV data has been carried out using the coupled-channels (CC) code FRESCO. Comparison of FRESCO calculations with those using the CC code CHUCK are presented. The CC calculations use an optical potential with double-folded (DF) real central, Woods-Saxon imaginary central, and Thomas real spin-orbit (SO) potentials. Calculations include reorientation terms and coupling to the first three excited states of $^{6}mathrm{Li}$ and the first two nonzerospin states of $^{12}mathrm{C}$. The $^{6}mathrm{Li}$ coupling strengths were fixed by the measured $^{6}mathrm{Li}$ excited-state cross sections. The elastic-scattering cross sections and A.P.'s are described well. The need for an explicit SO potential is apparent in the elastic and inelastic-scattering AP's ${mathit{iT}}_{11}$, more so at 30 MeV than at 50 MeV. The rank-2 AP's up to 50ifmmode^circelsetextdegreefi{} c.m. arise mainly from ground-state reorientation effects. The DF potential normalization constant N approaches unity for the 50 MeV data. At both energies, the $^{12}mathrm{C}$(${2}^{+}$) cross sections are underestimated at large angles, and the description of the $^{12}mathrm{C}$(${3}^{mathrm{ensuremath{-}}}$) cross sections is poor in detail. The $^{12}mathrm{C}$(${3}^{mathrm{ensuremath{-}}}$) AP's and the $^{12}mathrm{C}$(${2}^{+}$) ${mathit{iT}}_{11}$ are not reproduced at either energy. textcopyright{} 1996 The American Physical Society." @default.
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- W152152693 date "1996-09-01" @default.
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- W152152693 doi "https://doi.org/10.1103/physrevc.54.1267" @default.
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