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利用气泡探测器测量激光快中子
引用本文:赵磊,徐妙华,张翌航,张喆,朱保君,姜炜曼,张笑鹏,赵旭,仝博伟,贺书凯,卢峰,吴玉迟,周维民,张发强,周凯南,谢娜,黄征,仲佳勇,谷渝秋,李玉同,李英骏.利用气泡探测器测量激光快中子[J].物理学报,2018,67(22):222101-222101.
作者姓名:赵磊  徐妙华  张翌航  张喆  朱保君  姜炜曼  张笑鹏  赵旭  仝博伟  贺书凯  卢峰  吴玉迟  周维民  张发强  周凯南  谢娜  黄征  仲佳勇  谷渝秋  李玉同  李英骏
作者单位:1. 中国矿业大学(北京), 深部岩土力学与地下工程国家重点实验室, 北京 100083;2. 中国科学院物理研究所, 北京凝聚态物理国家研究中心, 北京 100190;3. 中国科学院大学物理科学学院, 北京 100049;4. 上海交通大学, IFSA协同创新中心, 上海 200240;5. 上海交通大学物理与天文学院, 上海 200240;6. 北京师范大学天文系, 北京 100875;7. 中国工程物理研究院激光聚变研究中心, 等离子体物理重点实验室, 绵阳 621900
基金项目:科学挑战计划(批准号:TZ2016005)、国家自然科学基金(批准号:11520101003,11535001,11574390)、国家重点基础研究发展计划(批准号:2013CBA01504)和中国科学院先导计划(批准号:XDB16010200,XDB07030300)资助的课题.
摘    要:在利用超强激光驱动中子源的研究和应用研究中,中子源的产额及其角分布至关重要.我们在星光Ⅲ号激光装置上采用气泡探测器对强激光驱动的中子源的产额及其角分布进行了测量.利用超强皮秒激光与碳氘薄膜靶相互作用产生高能氘离子束撞击次级碳氘靶,通过氘-氘核反应产生准单能快中子.实验发现中子束的发射具有一定的方向性,在入射氘离子的传输方向上中子束具有更高的强度,测量得到的中子束最大强度为5.13×107 n/sr.利用实验测量的氘离子能谱和角分布对中子束角分布进行了理论计算,结果与实验测量基本一致.

关 键 词:气泡探测器  快中子  角分布
收稿时间:2018-05-28

Laser fast neutron measured by bubble detector
Zhao Lei,Xu Miao-Hua,Zhang Yi-Hang,Zhang Zhe,Zhu Bao-Jun,Jiang Wei-Man,Zhang Xiao-Peng,Zhao Xu,Tong Bo-Wei,He Shu-Kai,Lu Feng,Wu Yu-Chi,Zhou Wei-Min,Zhang Fa-Qiang,Zhou Kai-Nan,Xie Na,Huang Zheng,Zhong Jia-Yong,Gu Yu-Qiu,Li Yu-Tong,Li Ying-Jun.Laser fast neutron measured by bubble detector[J].Acta Physica Sinica,2018,67(22):222101-222101.
Authors:Zhao Lei  Xu Miao-Hua  Zhang Yi-Hang  Zhang Zhe  Zhu Bao-Jun  Jiang Wei-Man  Zhang Xiao-Peng  Zhao Xu  Tong Bo-Wei  He Shu-Kai  Lu Feng  Wu Yu-Chi  Zhou Wei-Min  Zhang Fa-Qiang  Zhou Kai-Nan  Xie Na  Huang Zheng  Zhong Jia-Yong  Gu Yu-Qiu  Li Yu-Tong  Li Ying-Jun
Abstract:Neutron source has broad application prospects in crystallography, neutron irradiation, neutron therapy for cancer, and so on. As a new scheme to produce bright pulsed neutron source, the laser-driven neutron has attracted wide interest. In recent years, laser driven neutron sources have been extensively studied and the great progress has been made. Short pulsed laser driven neutron sources could be a compact and relatively cheap way to produce quasi-monoenergetic neutrons. The yields and the angular distributions of the laser-driven neutron sources are important in the research of laser-driven neutron sources and relevant applications. We conduct experimental investigation of this respect by using the XingGuang-Ⅲ high intense laser facility, which delivers synchronized picosecond and nanosecond laser pulses. The picosecond laser energy is 100 J, the pulse width is 1 ps, and the focusing spot diameter is 20 μm. At this time, the corresponding laser power density reaches 3×1019 W/cm2. A high-energy deuterium ion beam is produced by focusing the picosecond laser on a deuterated polyethylene foil, and the deuterium ion beam is incident on a secondary deuterated polyethylene planar target to activate the D-D reaction to obtain the neutron beam. In the experiment, the neutron yield and its angular distribution are measured by the different-sensitivity BD-PND bubble detectors, which are placed in the target chamber around the target. The emission of the neutron beam is found to be non-uniform. A maximum intensity of 5.13×107 n/sr is observed in the forward direction. The angular distribution of the neutron beam is theoretically calculated by taking into account the energy-angle cross section, the angular and energy distribution of the incident deuterium ion beam. The probability of the neutron energy-angle distribution in the laboratory system is obtained by the coordinate transformation from the probability in the center of mass frame. The results show good agreement with the experimental measurements. This experiment has a certain reference value in the practical application of D-D reaction neutron source.
Keywords:bubble detector  fast neutron  angular distribution
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