平坦效率对于实现光中子反应的单中子、双中子和三中子事件的区分和截面的计算非常关键。介绍了一种用于逆康普顿散射γ源(Shanghai Laser Electron Gamma Source,SLEGS)光中子(γ,n)截面测量的4π平坦效率3He中子探测器阵列的设计与模...平坦效率对于实现光中子反应的单中子、双中子和三中子事件的区分和截面的计算非常关键。介绍了一种用于逆康普顿散射γ源(Shanghai Laser Electron Gamma Source,SLEGS)光中子(γ,n)截面测量的4π平坦效率3He中子探测器阵列的设计与模拟。采用Geant4程序对平坦效率3He探测器的优化布局和效率进行了模拟,针对设计的由20只Φ50 mm×500 mm 5 cm 3He正比计数管和6只Φ25 mm×500 mm 3He正比计数管组成的4π平坦效率中子探测器,模拟给出探测器平均效率曲线在1 keV^6 MeV的效率为34.4%~45.9%。模拟中以209Bi靶为例,靶尺寸为Φ20 mm×4 mm,通过对产生中子的角分布,能谱的模拟计算,发现中子出射角度在90°对称,探测器的4π布局能够完全覆盖入射到聚乙烯慢化体的中子,出射中子能量随着中子分离能呈现出规律的变化关系;随着γ能量增加,出射道开放增多,出射中子的能量总是分布在1 keV^4 MeV之间,探测器阵列在这一能区的平均效率为40%~46%。展开更多
Large area plastic scintillation detectors are applied widely in modern physics labs due to the development of the time-of-flight technique. They are usually constructed with a module array design, such as the TOF Wal...Large area plastic scintillation detectors are applied widely in modern physics labs due to the development of the time-of-flight technique. They are usually constructed with a module array design, such as the TOF Wall. The performance of such detectors is excellent, but the number of electronics channels is quite large, and the operation and calibration are too complicated. As a result, a large area plastic scintillation detector with only 4 readout signals from the corners is constructed and developed as a simple TOF Wall at ETF in IMP.展开更多
文摘平坦效率对于实现光中子反应的单中子、双中子和三中子事件的区分和截面的计算非常关键。介绍了一种用于逆康普顿散射γ源(Shanghai Laser Electron Gamma Source,SLEGS)光中子(γ,n)截面测量的4π平坦效率3He中子探测器阵列的设计与模拟。采用Geant4程序对平坦效率3He探测器的优化布局和效率进行了模拟,针对设计的由20只Φ50 mm×500 mm 5 cm 3He正比计数管和6只Φ25 mm×500 mm 3He正比计数管组成的4π平坦效率中子探测器,模拟给出探测器平均效率曲线在1 keV^6 MeV的效率为34.4%~45.9%。模拟中以209Bi靶为例,靶尺寸为Φ20 mm×4 mm,通过对产生中子的角分布,能谱的模拟计算,发现中子出射角度在90°对称,探测器的4π布局能够完全覆盖入射到聚乙烯慢化体的中子,出射中子能量随着中子分离能呈现出规律的变化关系;随着γ能量增加,出射道开放增多,出射中子的能量总是分布在1 keV^4 MeV之间,探测器阵列在这一能区的平均效率为40%~46%。
文摘Large area plastic scintillation detectors are applied widely in modern physics labs due to the development of the time-of-flight technique. They are usually constructed with a module array design, such as the TOF Wall. The performance of such detectors is excellent, but the number of electronics channels is quite large, and the operation and calibration are too complicated. As a result, a large area plastic scintillation detector with only 4 readout signals from the corners is constructed and developed as a simple TOF Wall at ETF in IMP.
