• The angular distribution of 1H(6He,p)6He elastic scattering has been measured at Ec.m.=4.3 MeV by using a thick-target inverse kinematic method. The experimental differential cross sections are reproduced by the distorted-wave Born approximation calculation utilizing the CH89 global optical potential parameter set. The real part of CH89 is reduced comparing with other potentials, which may be attributed to the couplings necessary for the weakly bound nuclei.
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LIU Xin, WANG You-Bao, LI Zhi-Hong, JIN Sun-Jun, WANG Bao-Xiang, LI Yun-Ju, LI Er-Tao, BAI Xi-Xiang, GUO Bing, SU Jun, ZENG Sheng, YAN Sheng-Quan, LIAN Gang, HUANG Wu-Zhen and LIU Wei-Ping. Angular distribution of 6He+p elastic scattering[J]. Chinese Physics C, 2012, 36(8): 716-720. doi: 10.1088/1674-1137/36/8/006
LIU Xin, WANG You-Bao, LI Zhi-Hong, JIN Sun-Jun, WANG Bao-Xiang, LI Yun-Ju, LI Er-Tao, BAI Xi-Xiang, GUO Bing, SU Jun, ZENG Sheng, YAN Sheng-Quan, LIAN Gang, HUANG Wu-Zhen and LIU Wei-Ping. Angular distribution of 6He+p elastic scattering[J]. Chinese Physics C, 2012, 36(8): 716-720.  doi: 10.1088/1674-1137/36/8/006 shu
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Revised: 1900-01-01
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Angular distribution of 6He+p elastic scattering

    Corresponding author: WANG You-Bao,

Abstract: The angular distribution of 1H(6He,p)6He elastic scattering has been measured at Ec.m.=4.3 MeV by using a thick-target inverse kinematic method. The experimental differential cross sections are reproduced by the distorted-wave Born approximation calculation utilizing the CH89 global optical potential parameter set. The real part of CH89 is reduced comparing with other potentials, which may be attributed to the couplings necessary for the weakly bound nuclei.

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