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3篇 您的检索式：作者名="LiSonglin"

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		题名	作者	年代	出处	被引量
	1	Non-reproducibility of Cross Sections Measured in Dissipative Collisions of ^(19)F+^(93)Nb显示文摘Two independent measurements of excitation functions of the strongly dissipative collision for the same reaction system of 19F+93Nb have been carried out at the China Institute of Atomic Energy, Beijing. In these measurements, the 19F8+ beam was provided by the HI-13 tandem accelerator. The incident beam energies were varied from 102 to 108 MeV in steps of 250 keV. In both measurements the same accelerator	DongYuchuan WangQi TianWendong LiSonglin JiangZhonghe LiZhichang LuXiuqin ZhaoKui FuChangbo LiuJiancheng JiangHua HuGuiqing	2002	近代物理研究所和兰州重离子加速器实验室年报:英文版2002，，1：	0
	2	Development of Silicon Multi-strip Detector显示文摘Position sensitive detector is very important for nuclear physics experiment. There several techniques can be used to fabricate position sensitive detector, for example, Si-surface barrier method, diffusion method, ion implantation and planar process etc. Among all the techniques mentioned above planar process is the best one. We have developed batch of position sensitive detector -- silicon multi-strip detector by using planar process.	TanJilian JinGenming WangHongwei YuanXiaohua DuanLiming LiSonglin LuZiwei XuHushan NingBaojun TianDayu WangWei ZhangLu	2003	近代物理研究所和兰州重离子加速器实验室年报:英文版2003，，1：	0
	3	Excitation Function Measurement in Reaction of ^(19)F+^(27)A1显示文摘The measurement of excitation functions for the strongly dissipative collision with the reaction system of ^19F+^27Al has been carried out at the China Institute of Atoraic Energy, Beijing. The ^19F^8+ beam was extracted from the HI-13 tandem accelerator. The beam incident energies were varied from 110 to 118.75 MeV in steps of 250 keV. The self-supporting ^27A1 target foil with the thickness of 60μg/cm^2 was used. The detector arrangement is shown in Fig.1.	DongYuchuan WangQi LiSonglin DuanLimin WuHeyu XuHuagen ChenRuofu LiZhichang LuXiuqin ZhaoKui Zhouping LiuJiancheng	2003	近代物理研究所和兰州重离子加速器实验室年报:英文版2003，，1：	0

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