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• W2336393482 abstract "A set of global optical potential parameters describing the $A=3$ particles ($^{3}mathrm{He}$ and ${}^{3}mathrm{H}$) elastic scattering from $1p$-shell nuclei, $mathrm{HT}1p$, is obtained by simultaneously fitting 118 sets of experimental data of $^{3}mathrm{He}$ and ${}^{3}mathrm{H}$ elastic scattering from $^{9}mathrm{Be},{}^{10}mathrm{B},{}^{11}mathrm{B},{}^{12}mathrm{C},{}^{13}mathrm{C},{}^{14}mathrm{C},{}^{14}mathrm{N},{}^{15}mathrm{N},{}^{16}mathrm{O},{}^{17}mathrm{O}$, and ${}^{18}mathrm{O}$ with incident energies from $4ensuremath{le}Eensuremath{le}118.5$ MeV and 24 sets of elastic scattering data with the $^{6}mathrm{Li}$ and $^{7}mathrm{Li}$ targets from $3ensuremath{le}Eensuremath{le}44$ MeV. $mathrm{HT}1p$ is found to be superior to GDP08 [D. Y. Pang, P. Roussel-Chomaz, H. Savajols, R. L. Varner, and R. Wolski, Phys. Rev. C 79, 024615 (2009)], which is a systematic potential designed for the heavy-target region, in the reproduction of the angular distributions of elastic scattering cross sections of $^{3}mathrm{He}$ and ${}^{3}mathrm{H}$ from $1p$-shell nuclei at energies below 100 MeV. At energies above 100 MeV, GDP08 is found to be better than HT1p." @default.
• W2336393482 created "2016-06-24" @default.
• W2336393482 creator A5008766995 @default.
• W2336393482 creator A5022989303 @default.
• W2336393482 creator A5041826017 @default.
• W2336393482 date "2015-02-18" @default.
• W2336393482 modified "2023-10-17" @default.
• W2336393482 title "Optical model potential of<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML><mml:mrow><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mn>3</mml:mn></mml:mrow></mml:math>projectiles for<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML><mml:mrow><mml:mn>1</mml:mn><mml:mi>p</mml:mi></mml:mrow></mml:math>-shell nuclei" @default.
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• W2336393482 doi "https://doi.org/10.1103/physrevc.91.024611" @default.
• W2336393482 hasPublicationYear "2015" @default.
• W2336393482 type Work @default.
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