丝阵Z箍缩实验1维X光辐射功率分布

 在Angara-5-1联合实验中，利用条纹像机和光纤阵列实现时间分辨和1维空间分辨，得到了丝阵条纹像，观察到丝阵负载箍缩区X光辐射的1维轴向空间分布信息随时间的演化过程，考察了内爆的同步性和均匀性。通过对比不同结构负载内爆等离子体X光1维时空分布信息，发现由于内层等离子体对磁流体瑞利-泰勒不稳定性的抑制作用，(40+20)根双层钨丝阵比60根单层钨丝阵的内爆轴向同步性好，产生的X光辐射功率高；由于负载存在弯曲、断丝、扭曲等现象，(60+30)根双层钨丝阵比90根单层钨丝阵的轴向同步优势不明显；轴向同步性好与辐射功率高之间存在相关性；辐射波形前沿较快时，X光功率较高。     

单层钨丝阵Z箍缩内爆不稳定性特征实验研究

基于激光阴影像,研究了直径为8 mm的钨丝阵在滞止阶段的不稳定性发展。实验结果表明,在消融阶段早期,不稳定性扰动的主导波长为0.2 mm。在内爆后期和滞止阶段,不稳定主导波长迅速向长波长方向发展。在功率峰值前后,扭曲不稳定性特征开始出现,在滞止等离子体柱达到最小收缩直径后,辐射功率出现了明显下降。     

罗斯滤片法测量激光打靶X射线辐射通量

利用一套罗斯滤片系统测量激光轰击固体金属Ti平面靶产生的X射线辐射通量,系统包括两个相同的X射线探测器及相应滤膜。罗斯滤片法的优点在于利用相邻核素对X射线相似的阻止率,可滤出一个窄的能带并去除高能部分的干扰,获得了Ti平面靶K壳层X光辐射产额。实验结果表明:硬X射线能段在4.5~4.9keV之间的K壳特征辐射占优,连续谱所占份额较低(与晶体谱仪一致);随着激光能量的增加,特征辐射增加;激光强度接近2×1015 W/cm2时,能量转换效率出现峰值。     

X-ray observations of tungsten wire array Z-pinch implosions on QiangGuang-1 facility

Z-pinch experiments with two arrays consisting, respectively, of 32 4-μm- and 6-μm-diameter tungsten wires have been carried out on QiangGuang-1 facility with a current rising up to 1.5MA in 80ns. At early time of implosion, x-ray framing images show that the initial emission comes from the central part of arrays, and double clear emission rings, drifting to the anode and the cathode at 5×10⁶cm/s and 2.4×10⁷cm/s respectively, are often produced near the electrodes. Later, in a 4-μm-diameter tungsten wire array, filamentation caused by ohmic heating is prominent, and more than ten filaments have been observed. A radial inward shift of arrays starts at about 30\,ns earlier than the occurrence of the x-ray peak power for both kinds of arrays, and the shrinkage rate of emission region is as high as 1.7×10⁷cm/s in a 4-μm-diameter tungsten wire array, which is two times higher than that in a 6-μm one. Emission from precursor plasmas is observed in implosion of 6-μm-diameter tungsten wire arrays, but not in implosion of a 4-μm-diameter tungsten wire array. Whereas, in a 4-μm-diameter tungsten wire array, the soft x-ray emission shows the growth of m=1 instability in the plasma column, which is caused by current. The reasons for the discrepancy between implosions of 4-μm- and 6-μm-diameter tungsten wire arrays are explained.     

用于n,γ混合场的新型脉冲中子探测器研究

新型脉冲中子探测器采用特殊工艺将两个PIN半导体组合而成.利用脉冲γ辐射研究了探测器对γ的响应；利用脉冲中子源研究了探测器对DT中了的响应，并与闪烁探测器进行了比较 .结果表明：脉冲中子探测器对脉冲γ辐射基本不灵敏，对脉冲中子辐射的灵敏程度依赖于中子辐射体，是一种用于n，γ混合脉冲辐射场中子测量的新型探测器. 关键词： 硅半导体 差分补偿 脉冲中子探测器 n γ混合场     

含三苯胺的1,8-萘酰亚胺衍生物的合成及光谱和电化学性能研究

通过Suzuki偶联反应合成了一系列含三苯胺的1,8-萘酰亚胺衍生物，并进行了表征及光谱和电化学性能研究。研究表明该类化合物的荧光波长在584~610nm，位于橙色区。三苯胺的引入降低了化合物的HOMO值，有利于空穴的注入。     

对γ不灵敏的PIN脉冲中子探测器

将PIN半导体制作成特殊组合结构的PIN脉冲中子探测器,利用三通道装置产生的γ脉冲和中子发生器DT反应产生的14MeV中子脉冲对探测器进行了研究.结果表明:PIN脉冲中子探测器对脉冲γ辐射不灵敏,对脉冲中子辐射的灵敏程度依赖于中子辐射转换靶,探测器的信噪比达到30∶1,是一种在中子、γ混合脉冲辐射场中测量脉冲中子的新型探测器     

Z-pinch内爆等离子体时空分辨诊断技术

 为了深入认识和理解Z-pinch物理机制并对物理实验进行优化设计，需要研究内爆等离子体及其辐射的时空分布特性诊断技术，建立诊断装置与设备，通过实验研究等离子体内爆时间过程及其空间分布特性，利用所获得的实验诊断数据校核数值模拟程序。简要介绍近几年开展的X光空间积分功率谱测量、X光时间积分针孔照相、X光时分幅针孔照相、X光时间分辨1维空间分布、紫外探针阴影照相等时空分辨诊断技术研究工作，并给出在1~3 MA电流驱动装置上进行的喷气和丝阵内爆实验中获得的部分时空分辨诊断结果，包括辐射功率、拉链速度、内爆速度、收缩比等。     

丝阵Z箍缩1维X射线辐射功率分布的数据处理

 在丝阵Z箍缩实验中利用CCD记录X射线辐射功率的1维时空分布图像，对光纤传输效率、图像聚焦、MCP与CCD的耦合效率等因素造成的图像失真进行了处理，利用实验实测的单光纤点扩展图像和光传输效率曲线对辐射功率分布图像进行处理，并修正光纤传输效率以及MCP和CCD间耦合效率不均匀性的影响以还原X射线辐射功率的1维空间分布信息。处理后将图像沿空间积分获得了与X射线功率谱仪相吻合的X射线辐射功率脉冲波形，同时不同发次由两系统得到的X射线波形的前沿之间也表现出了良好的一致性。     

Experimental study on imploding characteristics of wire-array Z pinches on Qiangguang-1 facility

To investigate the imploding characteristics of cylindrical wire array, experiments with load current varying from 1.5\,MA to 1.7\,MA were carried out on the Qiangguang-1 facility. The complicated temporal-spatial distribution of x-ray radiation was measured by the one-dimensional (1D) x-ray imaging system. Other diagnostic equipments including the x-ray power meter (XRPM) and the time-integrated pinhole camera were used to record time-resolved x-ray power pulse and pinhole x-ray images. Analysis shows that the fast leading edge of the local x-ray radiation pulse is of primary importance in sharpening x-ray power pulse rather than the temporal synchrony and the spatial uniformity of implosion. Experimental results indicated that the better axial imploding synchrony, the faster the increase of x-ray power for an array consisting of 32 tungsten wires of 5\mum diameter than for the others, and the higher the x-ray radiation power with maximal convergence ratio (r_0/r_1) of 10.5. A `zipper-like' effect of x-ray radiation extending from the anode to the cathode was also observed.