用于照射量仪校准工作的监测电离室

本文描述用于照射量仪校准工作的薄窗监测电离室的结构、性能及使用方法，就重复性而言，电离室的读数在0．2％以内相符；用于校准现场仪器时，在中等过滤的情况下误差小于1％，重过滤下不大于2％。     

电流电离室教学实验装置的研制

介绍流气式电流电离室实验装置的制作,测量了该电离室的饱和特性、轴向均匀性等性能参数,将该电离室用于核与粒子物理实验教学中,取得了良好效果。     

用于快中子探测的裂变电离室实验及模拟结果比较(英文)

本文报道了一种用于快中子测量的裂变电离室的实验及模拟结果对比,该电离室的裂变材料为238U,分别电镀在电离室的阳极和阴极。裂变电离室通常有三种工作模式:脉冲模式、均方电压模式和电流模式,从而在大动态范围内实现中子注量测量。我们利用252Cf中子源对工作在脉冲模式的裂变电离室效率进行了测量,同时为了评估均方电压模式和电流模式,测量了裂变电离室在不同气压下的脉冲幅度,并通过Geant4蒙特卡罗软件对裂变电离室的脉冲幅度进行了模拟。模拟可以解释实验结果,当工作气压是2.64×105 Pa时探测效率最高[（4.30±0.7）×10-7],且裂变碎片能谱清晰,表明裂变电离室可以工作在不同模式下。     

用于反应堆中子/γ 射线混合场测量的涂硼电离室性能

近年来,涂硼电离室已逐渐成为核反应堆周围大通量中子/γ射线混合场监测的辐射探测器之一. 研制了一种高灵敏度涂硼电离室,并给出了其内部结构.用fA级弱电流放大器测得: 当涂硼电离室的工作电压在700 V以下时,漏电流小于1.0 pA; 用Am-Be中子源辐照时测得涂硼电离室的电流曲线坪长为500 V, 坪斜为3.72×10^-4 V^-1;当涂硼电离室的工作电压为400 V时, 对应漏电流为0.4 pA.测试表明涂硼电离室中子信号电流与辐照源的相对位置有关, 将Am-Be中子源置于距石蜡慢化体底部8 cm时,测得中子信号电流最大值为2.0 pA. 用¹³⁷Cs和⁹⁰Sr辐照时测得涂硼电离室γ射线信号电流为 1.0---2.0 pA,但在γ射线场中坪特性不如中子场中坪特性明显. 电离室中子探测灵敏度达1.0×10^-15 Acm²s量级, γ射线探测灵敏度达9.0× 10^-22 Acm²s·eV^-1量级. 这种涂硼电离室漏电流小、灵 敏度高、坪特性好,可用于反应堆周围的中子/γ射线混合场测量.     

入射能量为5．1MeV中子~（58）Ni（n，α）~（55）Fe反应截面和出射

用屏栅电离室测量了入射中子能量为５．１ＭｅＶ的５８Ｎｉ（ｎ，α）５５Ｆｅ核反应的α粒子角分布，２３８Ｕ裂变电离室作中子注量率的测量，测得该能点５８Ｎｉ（ｎ，α）５５Ｆｅ的总截面为（４７．４±５．０）ｍｂ．用中国核数据中心推荐的理论计算程序ＵＮＦ计算了在１—８ＭｅＶ能区５８Ｎｉ（ｎ，ｐ）５８Ｃｏ，５８Ｎｉ（ｎ，α）５５Ｆｅ的反应截面和入射中子能量为５．１ＭｅＶ的５８Ｎｉ（ｎ，α）反应角分布．理论和测量数据的比较说明，用复合核模型来描写该能点的角分布是可行的．     

一种多阳极横向场电离室

描述了一种将用于兰州放射性束流线较重离子鉴别的多阳极横向场电离室.对其性能进行了初步测试,得到该电离室有较长的坪区和较好的能量分辨.在10⁴Pa的P10工作气体(10%CH₄+90%Ar)下,坪区长度为700V.对²⁴⁴Cm α放射源,在第4片阳极对应的灵敏区域能量损失为1.30MeV,能量分辨41.1keV,相对能量分辨约3.16%。     

真空紫外波段绝对光强的测量研究

介绍了利用双极型稀有气体电离室进行真空紫外波段(12~34nm)绝对光强测量的方法,并对Ar在12~34nm波段的电离吸收截面进行了测量。讨论了在利用稀有气体电离室进行绝对光强测量时,二次电离对测量结果的影响。通过建立适当的数学模型来确定二次电离系数。     

屏栅电离室+△E-E望远镜探测器系统

研制了屏栅电离室+△E-E望远镜探测器系统,系统的屏栅电离室用来测定252Cf自发裂变碎片的能量和相对于探测器系统轴线的发射角,与屏栅电离室耦合安装的△E-E望远镜探测器由一个薄的屏栅电离室(气体△E)和一个金硅面垒探测器(E)组成,用来确定互补碎片的电荷.用本系统对252Cf自发裂变碎片电荷分布进行了4个参数的关联测量,结果表明,这个探测器系统的电荷分辨能力Z/△Z好于40:1.     

屏栅电离室+△E-E望远镜探测器系统

研制了屏栅电离室+△E-E望远镜探测器系统,系统的屏栅电离室用来测定252Cf自发裂变碎片的能量和相对于探测器系统轴线的发射角,与屏栅电离室耦合安装的△E-E望远镜探测器由一个薄的屏栅电离室(气体△E)和一个金硅面垒探测器(E)组成,用来确定互补碎片的电荷.用本系统对252Cf自发裂变碎片电荷分布进行了4个参数的关联测量,结果表明,这个探测器系统的电荷分辨能力Z/△Z好于40:1.     

一种用于RIBLL2的纵向场多次取样型电离室

为兰州第二条放射性束流线（RIBLL2）研制了一台用于ΔE测量的纵向场多次取样型电离室。 利用3组分α源（239Pu为3.435 MeV, 241Am为3.913 MeV, 244Cm为4.356 MeV）对取样单元进行了测试, 确定了电离室的最佳工作电压为－500 V, 沉积能量为3.435 MeV时, 取样单元的能量分辨为271.4 keV(FWHM)。 利用Geant4对此电离室的整体性能进行了模拟, 表明可以对Z≥4的离子实现较好的粒子鉴别。 A longitudinal field MUltiple Sampling Ionization Chamber (MUSIC), which makes multiple measurements of energy loss for very high energy heavy ions at RIBLL2, has been constructed and tested with 3 constituent α source （239Pu: 3.435 MeV, 241Am: 3.913 MeV, 244Cm: 4.356 MeV）. The voltage plateau curve has been plotted and －500 V is determined as a proper work voltage. The energy resolution is 271.4 keV FWHM for the sampling unit when 3.435 MeV energy deposited. A Geant4 Monte Carlo simulation is made and it indicates the detector can provide unique particle identification for ions Z≥4.     

Study of the energy response of high pressure ionization chamber for high energy gamma-ray

The energy response calibration of the commonly used high pressure ionization chamber is very difficult to obtain when the gamma-ray energy is more than 3 MeV. In order to get the calibration of the higher part of the high pressure ionization chamber, we use the Fluka Monte Carlo program to perform the energy response in both the spherical and the cylindrical high pressure ionization chamber which are full of argon gas. The results compared with prior study when the gamma-ray energy is less than 1.25 MeV. Our result of Monte Carlo calculation shows agreement with those obtained by measurement within the uncertainty of the respective methods. The calculation of this study is significant for the high pressure ionization chamber to measure the high energy gamma-ray.     

Multi-purpose explosion chamber with sound muffling and vibration cutting means

Abstract

An explosion chamber is operating for more than 13 years successfully. The chamber is used for procucing wBN powder and various dynamic high pressure experiments. The capacity of the chamber is 200 cubic meter by volume and 10 kg by the quantity of the explosives to be exploded. Safety means are equipped sequentially, transmitted sound level is less than 65 db at 60 m point from the chamber and earth vibrations cannot be detected at its periphery. The strength of the chamber was designed by simple static gas pressure model.     

Study of the energy response of high pressure ionization chamber for high energy gamma-ray

The energy response calibration of the commonly used high pressure ionization chamber is very difficult to obtain when the gamma-ray energy is more than 3 MeV.In order to get the calibration of the higher part of the high pressure ionization chamber,we use the Fluka Monte Carlo program to perfclrm the energy response in both the spherical and the cylindrical high pressure ionization chamber which are full of argon gas.The results compared with prior study when the gamma-ray energy is less than 1.25 MeV.Our result of Monte Carlo calculation shows agreement with those obtained by measurement within the uncertainty of the respective methods.The calculation of this study is significant for the high pressure ionization chamber to measure the high energy gamma-ray.     

Monte Carlo simulation of exposure factor

In this paper, we simulate the exposure factor by a simple model of a free-air ionization chamber with the Monte Carlo programme Geant4. Special emphasis is placed on the discussion of the exposure factor related to parameters of the chamber model. The reason for the variation in exposure factor with incident ray energy is also analysed in terms of reaction cross section for different types of reactions. The obtained results indicate that our simulation is accurate in the calculation of the exposure factor and can serve as a reference in designing air ionization chambers.     

绝对吸收式激光能量计高准确度校准技术研究

采用量热法的高能激光能量计用于测量能量大于50 kJ的连续波高能激光能量,通常用已知功率的连续激光开展激光能量计的光电校准需要激光照射时间超过20 min,而由于热损失等原因,进行长时间激光能量校准时,校准不确定度高达12%。以量热式平面吸收高能激光能量计为模型,从理论上分析了热辐射、热对流对连续波高能激光能量测量结果的影响,得到了较准确的平面吸收腔激光能量计冷却数学模型,实现了能量计热损失补偿,并通过建立相应的实验装置验证了该模型,用其对装置的测量结果加以修正,可使光电校准的测量不确定度减小到1%以下。     

Design of a reverberant chamber for noise exposure experiments with small animals

Previous work on the acoustic design of small reverberant chambers for studies on laboratory animals has paid, in general, more attention to the frequency response at certain points in their interior. These designs aimed to provide a frequency response as flat as possible at the receivers, thus avoiding unpleasant spectral coloration effects. However, an equally important, and frequently neglected, aspect is to set an acoustic field as spatially uniform as possible inside the zone where the animals are to be placed during the exposure to noise. Here, an optimization procedure is described to calculate the proportions of the chamber dimensions that confers the highest sound level with the minimum mean squared deviation averaged in a given area inside the chamber. In addition, new stimuli have been designed with a high-pass filtering and linear with frequency gain. These stimuli were intended to adapt the characteristics of the exposing noise to the rodent hearing spectrum, displaced toward higher frequencies than the hearing frequency band of humans.     

薄壁快脉冲252Cf裂变电离室的研制及性能测试

介绍了用于中子探测器效率刻度的薄壁快脉冲252Cf裂变电离室。 在用飞行时间法测量中子能谱时, 该裂变电离室能够给出252Cf裂变中子发射时刻信号, 输出脉冲上升时间约为5.5 ns, 电离室由厚度为0.15 mm的不锈钢构成。 测试结果表明, 对裂变碎片的探测效率为99.2%, α粒子脉冲幅度和碎片脉冲幅度可清晰分开。A thin wall, fast pulse 252Cf ionization chamber, which was designed for calibrating efficiency of neutron detectors, was described. The ionization chamber can be used as the start detector in time of flight measurements of the 252Cf fission neutron spectrum. The chamber is composed of 0.15 mm thick stainless steel, the rise time of pulse signals is about 5.5 ns. As the test result shows, the detection efficiency of fission fragments is 99.2%, and pulse signals caused by fissions are distinguished clearly from those caused by α decays.     

Improved design and construction of an ionization chamber for the CSNS beam loss monitor (BLM)

Based on the first ionization chamber (IC) prototype, the structure, working gas component and electrode material of the IC are improved. The test of the improved IC shows that the plateau length is about 2000 V, the plateau slope is less than 0.2%/100 V, the sensitivity is 19.6 pA/rad·h^-1, the up-limitation of the linearity can be up to 3.6×10⁵ rad/h, and the applied voltage can be operated to 3500 V. The test results show that the performance of the improved IC meets the requirements of the beam loss monitor.