Three different types of experiments have been performed to explore the complete and incomplete fusion dynamics in heavy-ion collisions. In this respect, first experiment for the measurement of excitation functions of the evaporation residues produced in the Ne-20+Ho-165 system at projectile energy ranges approximate to 2-8 MeV/nucleon has been done. Measured cumulative and direct cross-sections have been compared with the theoretical model code PACE-2, which takes into account only the complete fusion process. It has been observed that, incomplete fusion fraction is sensitively dependent on projectile energy and mass asymmetry between the projectile and the target systems. Second experiment for measuring the forward recoil range distributions of the evaporation residues produced in the Ne-20+Ho-165 system at projectile energy approximate to 8 MeV/nucleon has been done. It has been observed that, some evaporation residues have shown additional peaks in the measured forward recoil range distributions at cumulative thicknesses relatively smaller than the expected range of the residues produced via complete fusion. The results indicate the occurrence of incomplete fusion involving the breakup of Ne-20 into He-4+O-16 and/or Be-8+C-12 followed by one of the fragments with target nucleus Ho-165. Third experiment for the measurement of spin distribution of the evaporation residues produced in the O-16+Sn-124 system at projectile energy approximate to 6 MeV/nucleon, showed that the residues produced as incomplete fusion products associated with fast alpha and 2 alpha-emission channels observed in the forward cone, are found to be distinctly different from those of the residues produced as complete fusion products. The spin distribution of the evaporation residues also inferred that in incomplete fusion reaction channels input angular momentum (J(0)) increases with fusion incompleteness when compared to complete fusion reaction channels. Present observation clearly shows that the production of fast forward alpha-particles arises from relatively larger angular momentum in the entrance channel leading to peripheral collision.
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Zhengzhou Univ, Dept Phys, Zhengzhou 450001, Peoples R ChinaZhengzhou Univ, Dept Phys, Zhengzhou 450001, Peoples R China
Wang, Bing
Wen, Kai
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Chinese Acad Sci, Inst Theoret Phys, CAS Key Lab Frontiers Theoret Phys, Beijing 100190, Peoples R China
Univ Tsukuba, Fac Pure & Appl Sci, Tsukuba, Ibaraki 3058571, JapanZhengzhou Univ, Dept Phys, Zhengzhou 450001, Peoples R China
Wen, Kai
Zhao, Wei-Juan
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Zhengzhou Univ, Dept Phys, Zhengzhou 450001, Peoples R ChinaZhengzhou Univ, Dept Phys, Zhengzhou 450001, Peoples R China
Zhao, Wei-Juan
Zhao, En-Guang
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Chinese Acad Sci, Inst Theoret Phys, CAS Key Lab Frontiers Theoret Phys, Beijing 100190, Peoples R China
Ctr Theoret Nucl Phys, Natl Lab Heavy Ion Accelerator, Lanzhou 730000, Peoples R ChinaZhengzhou Univ, Dept Phys, Zhengzhou 450001, Peoples R China
Zhao, En-Guang
Zhou, Shan-Gui
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Chinese Acad Sci, Inst Theoret Phys, CAS Key Lab Frontiers Theoret Phys, Beijing 100190, Peoples R China
Ctr Theoret Nucl Phys, Natl Lab Heavy Ion Accelerator, Lanzhou 730000, Peoples R China
Univ Chinese Acad Sci, Sch Phys, Beijing 100049, Peoples R China
Hunan Normal Univ, Synerget Innovat Ctr Quantum Effects & Applicat, Changsha 410081, Hunan, Peoples R ChinaZhengzhou Univ, Dept Phys, Zhengzhou 450001, Peoples R China