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Common optical potential and peripheral processes between<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mn>1</mml:mn><mml:mi>p</mml:mi></mml:math>-shell nuclei

C. W. TowsleyCyclotron Institute, Texas A & M University, College Station, Texas 77843P. K. BindalCyclotron Institute, Texas A & M University, College Station, Texas 77843Katsunori KuboCyclotron Institute, Texas A & M University, College Station, Texas 77843K.G.M. NairCyclotron Institute, Texas A & M University, College Station, Texas 77843K. NagataniCyclotron Institute, Texas A & M University, College Station, Texas 77843
1977en
ABI

Annotatsiya

Elastic and inelastic scattering were measured for beams of 100-MeV $^{10}\mathrm{B}$ and 155-MeV $^{14}\mathrm{N}$ on targets of $^{12}\mathrm{C}$ and $^{16}\mathrm{O}$. These data and previously measured one-nucleon transfer data for the same four incident channels were analyzed simultaneously. A single set of optical potential parameters, fitting all the elastic scattering data, was obtained. Distorted-wave Born approximation analyses of the inelastic and transfer reactions were also done with this potential, resulting in good fits to the data. The common features in all of these peripheral collisions are emphasized.NUCLEAR REACTIONS NUCLEAR STRUCTURE $^{12}\mathrm{C}$($^{10}\mathrm{B}$, $^{10}\mathrm{B}$), $^{12}\mathrm{C}$($^{10}\mathrm{B}$, $^{10}\mathrm{B}$\ensuremath{'}), $^{16}\mathrm{O}$($^{10}\mathrm{B}$, $^{10}\mathrm{B}$), $^{16}\mathrm{O}$($^{10}\mathrm{B}$, $^{10}\mathrm{B}$\ensuremath{'}), $E=100$ MeV; $^{12}\mathrm{C}$($^{14}\mathrm{N}$, $^{14}\mathrm{N}$), $^{12}\mathrm{C}$($^{14}\mathrm{N}$, $^{14}\mathrm{N}$\ensuremath{'}), $^{16}\mathrm{O}$($^{14}\mathrm{N}$, $^{14}\mathrm{N}$), $^{16}\mathrm{O}$($^{14}\mathrm{N}$, $^{14}\mathrm{N}$\ensuremath{'}), $E=155$ MeV; measured $\ensuremath{\sigma}(\ensuremath{\theta})$; optical potentials, EFR-DWBA analyses extracted $\ensuremath{\beta}'\mathrm{s}$.

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