组合式Si-PIN 14 MeV中子探测器

提出了一种在多片Si-PIN探测器中间用2mm厚的聚乙烯作为灵敏度增强介质，采用加法电路模式进行信号输出的组合式新型DT聚变中子(14MeV)探测技术原理. 这种组合的主要特点有： 1)大幅度提高了Si-PIN探测器的中子灵敏度和测量统计性； 2)提高了探测器的n/γ分辨本领； 3)在实现多个探测器信号相加的同时，组合探测器相对于单片探测器时间响应没有明显改变. 从实验及理论上对组合探测器的14MeV中子及1.25MeV γ灵敏度、n/γ分辨，时间特性和测量统计性进行了研究. 关键词： Si-PIN半导体探测器 灵敏度 n/γ分辨 时间响应     

浅海声场中拖曳线列阵常规波束形成器对本舰噪声的接收响应

以浅海声场模型为基础,通过计算机仿真,研究了拖曳线列阵对本舰噪声的接收响应,对接收本舰噪声的最大阵输出偏离指向本舰的端射方向这一现象给出了合理的解释。这一结果对于拖曳线列阵抑制本舰噪声的研究,以及在浅海环境的正确应用,具有重要意义。     

CVD金刚石薄膜探测器性能研究

通过实验测量和理论分析, 从载流子动力学角度研究了用于脉冲辐射探测的CVD金刚石薄膜探测器的适用结构、电荷收集效率和时间响应性能. 结果表明, CVD金刚石薄膜可以制成均匀型结构的探测器; 薄膜中的缺陷会降低探测器的电荷收集效率, 探测器的电荷收集效率随场强增大而增大直至饱和. 已研制的CVD金刚石探测器电荷收集时间可达719ps, 在2.5V/μm场强下达到饱和, 电荷收集效率 达60.5%; 晶格散射是影响探测器时间响应的主要因素, 选用大晶粒甚至单晶金刚石薄膜可以提高探测器时间响应.     

~(133)Ba面源效率转移法刻度~(133)Xe气体源HPGe探测效率

提出使用面源进行效率转移法刻度133 Xe气体体源的探测效率。使用133 Ba面源模拟刻度放射性133 Xe气体体源的探测效率,在刻度的过程中利用137 Cs与133Ba的峰效率比值及133 Ba面源远端无符合相加效应,137 Cs能峰远近都无符合相加效应等,结合软件模拟建立远近距离峰效率比值的关系,来解决133 Ba的符合相加效应。最后,使用面源效率转移法进行气体体源效率刻度,转移法刻度结果和面源模拟法刻度计算值的偏差在±1%以内。     

介质型脉冲高能中子探测器

首次报道一种基于反冲质子法和高速带电粒子在物质表面引起二次电子发射的高能中子探测方法,研制成功的新一代强流脉冲高能中子探测器,即介质型脉冲高能中子探测器.与传统的强流脉冲中子探测器相比,该探测器对中子的探测及信号的传输过程是在介质中完成的,因而不需要真空和高压也可以正常工作,并具有多项优异的物理性能.该探测器的输出信号来自于高能中子在聚乙烯转换靶产生的高能反冲质子和这些质子穿越电荷收集极表面时产生的部分二次电子.选择适当的卡阈吸收片和电荷收集极材料,二次电子在探测灵敏度中的份额及其随能量的变化可由实验测定.     

浅海声速剖面的匹配波束反演方法

为了快速反演获得浅海声速剖面,利用匹配波束构造了反演代价函数,在此基础上研究了浅海声速剖面的匹配波束反演方法(MBI)。并运用东中国海的实验数据进行实际反演,验证了MBI的可行性和鲁棒性。利用垂直线列阵接收的29个不同位置的爆炸声信号进行了声速剖面反演, MBI反演的结果与实验中直接测量的声速剖面一致,且反演声速剖面的均方根误差小于2 m/s。研究结果表明,MBI比常规匹配场反演(MFI)获得浅海声速剖面更快速、更准确,并且对底质参数的失配具有较高的鲁棒性。     

金刚石膜探测器研制

采用直流电弧等离子喷射(DC arc plasma jet)CVD(chemical vapour deposition)工艺制成的金刚石薄膜，研制成功MSM(metal-semiconductor-metal)型CVD金刚石脉冲辐射探测器.对制作的金刚石薄膜材料及探测器有关性能进行了测量，结果表明，采用Raman shift<4.5cm^-1的金刚石薄膜制成的探测器，可满足亚纳秒脉冲辐射探测的要求.由于其独特的物理性能，在制作成本合理的情况下，在脉冲辐射测量中可取代Si-PIN探测器. 关键词： CVD 金刚石薄膜 辐射探测器     

A CVD diamond film detector for pulsed proton detection

A chemical vapour deposition （CVD） diamond film detector was prepared and the main characteristics for pulsed proton detection were studied at Beijing Tandem Accelerator. The result shows that the charge collection efficiency of the detector increases with increasing electric field intensity and reaches to 9.44% at 5 V/μm with the charge collection distance of 15.9 μm. The relationship between the sensitivity of the detector and proton energy is consistent with the Monte Carlo （MC） simulation result. Its plasma time for a pulse with 4.85×10^5 protons is 1l.2ns. The dose threshold for onset of damage under 9MeV proton irradiation in the detector is about 10^13 cm^-2. All of the results show that a CVD diamond detector has fast time response and high radiation hardness, and can be used in pulsed proton detection.     

Properties study of ZnO:Ga crystal on pulsed radiation detections

In this paper, properties on pulsed radiation detections of ZnO：Ga crystal grew by a magnetron sputtering method were studied. The time response to pulsed laser, pulsed hard X rays and single α particles, the energy response to pulsed hard X ray, the scintillation efficiency to γ rays, the response to pulsed proton, and the relations of the light intensity varied with the proton energy were measured and analyzed in detail. Results show that the ZnO：Ga crystal has potential applications in the regime of pulse radiation detection.     

Experimental study on scintillation efficiency of ZnO:In to proton response

Film ZnO:In crystal is a good candidate for a scintillation recoil proton neutron detection system and the response of ZnO:In to protons is a crucial point. The energy response of ZnO:In to mono-energetic protons in the range of 10 keV-8 MeV was measured. The experiment was carried out in current mode, and Au foil scattering was employed, where the forward scattering protons were used for exciting the sample, and the backward scattering protons were used for monitoring the beam intensity. According to the result, the yield of light non-linearly depends on proton energy, and drops significantly when proton energy is low. The scintillation efficiency as a function of proton energy was obtained, which is very useful for researching the scintillation recoil proton neutron detection system.