Investigation of breakup process in 9 Be( a ,n) 12 C reaction

被引:0
|
作者
Datta, Ritika [1 ,2 ]
Banerjee, K. [2 ,3 ]
Chatterjee, Sujoy [3 ]
Santra, Rajkumar [3 ]
Shil, R. [4 ]
Manna, S. [2 ,3 ]
Roy, Pratap [2 ]
Rana, T. K. [2 ]
Mukherjee, G. [2 ]
Ghosh, T. K. [2 ]
Roy, A. S. [1 ,2 ]
Sen, A. [2 ,3 ]
Kundu, S. [2 ,3 ]
Dey, Anirudhha [4 ]
Karmakar, P. [2 ,3 ]
Pandit, D. [2 ,3 ]
Bakshi, A. K. [1 ,2 ]
Sapra, B. K. [1 ,2 ]
Bhattacharyya, C. [3 ]
机构
[1] Bhabha Atom Res Ctr, Mumbai 400085, India
[2] Homi Bhabha Natl Inst, Mumbai 400094, India
[3] Variable Energy Cyclotron Ctr, 1-AF Bidhannagar, Kolkata 700064, India
[4] Visva Bharati, Dept Phys, Santini Ketan 731235, India
关键词
Neutron spectroscopy; Breakup; Resonance reaction; FLUKA; TALYS; PHITS; NEUTRON SOURCE; CROSS-SECTION; CODE SYSTEM; SPECTRA;
D O I
10.1016/j.nuclphysa.2024.122890
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
Neutron energies and angular distributions were measured in 9 Be(a,n) 12 C reaction for a energies of 5.5 and 6.5 MeV. Three major neutron groups were observed in the spectrum, which correspond to the ground and first two excited states of 12 C. Measured data could only be explained by the TALYS calculation if reaction at more than one location within the target is considered for a given beam energy. The preferred locations are driven by the resonance energy levels existing in 13 C. Neutron yield due to the 9 Be breakup process was determined which is found to be 12.6 +/- 0.2% and 18.4 +/- 0.5% of the total reaction cross-section for 5.5 and 6.5 MeV respectively.
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页数:11
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