The progress of nuclear pumped laser in CFBR-Ⅱ reactor

Development of nuclear pumped lasers (NPL) in the CFBR-Ⅱ reactor is briefly reviewed. The results ofthe two NPL experiments in CFBR-Ⅱ reactor are described. The first one focused on the principle ofnuclear pumped laser, and 4-mW laser output power achieved. The second NPL experiment focused onthe small signal gain and the efficiency of the nuclear pumped He-Ar-Xe gas mixture at 1.73 μm. Themaximum laser power measured to be 45 mW when thermal neutron flux rate is 6.9 × 10 14 cm-2 @ s-1.The small signal gain at 1.73μm by the Rigrod analysis method is to be 0.24%.cm-1, and the saturationintensity is fitted to be 36 W/cm2.     

CFBR-Ⅱ快中子脉冲堆及其应用

本文简介ＣＦＢＲ－Ⅱ堆的结构、主要性能指标及应用前景和相应的配套设施． The main specifications, structure and applications of CFBR-Ⅱ are simply introduced in this paper. The reactor s installations and fscilities are also mentioned.     

CFBR—Ⅱ快中子脉冲堆及其应用

本文简介ＣＦＢＲ－Ⅱ堆的结构、主要性能指标及应用前景和相应的配套设施。     

堆泵浦~3He－Ar－Xe体系的激光原理性实验

介绍了在ＣＦＢＲ－Ⅱ脉冲堆上进行的￣３Ｈｅ─Ａｒ─Ｘｅ体系的激光演示实验。当热中子注量率６×１０￣（１４）／ｃｍ￣２·ｓ，气体组配￣３Ｈｅ：Ａｒ：Ｘｅ＝３４．７：３４．７：０．２６７（ｋＰａ）时，获得波长λ＝１．７３μｍ、脉宽（ＦＷＨＭ）平均值７３８μｓ、峰值功率为毫瓦级的激光输出。同时对测得的光信号及其特性进行了分析。     

The progress of nuclear pumped laser in CFBR-II reactor

Development of nuclear pumped lasers (NPL) in the CFBR-Ⅱ reactor is briefly reviewed. The results of the two NPL experiments in CFBR-Ⅱ reactor are described. The first one focused on the principle of nuclear pumped laser, and 4-mW laser output power achieved. The second NPL experiment focused on the small signal gain and the efficiency of the nuclear pumped He-Ar-Xe gas mixture at 1.73 μm. The maximum laser power measured to be 45 mW when thermal neutron flux rate is 6.9 × 1014 cm-2 · s-1. The small signal gain at 1.73 μm by the Rigrod analysis method is to be 0.24%-cm"1, and the saturation intensity is fitted to be 36 W/cm2.     

新建堆厅的密封包容性检测

新建堆厅必须具有很好的密封包容性，即对放射性气溶胶具有小的泄漏率（常压下约10^-2／d；超压保持约1h，超压情况下的泄漏率是常压下的约10倍）。在堆厅建造完成后，用实验来检验其是否满足设计要求。采用工程模拟性的SF6气体作为示踪剂对3个堆厅的密封包容性进行了检测，该方法是研究气体扩散、混合、渗漏及泄漏和传输等气体动力学特征的有效方法。SF6气体示踪检漏的基本原理是在堆厅内具有所需压力后，在堆厅内迅速释放一定量的SF6气体，然后将堆厅内取样点处的气样通过管道直接引入气相色谱进样系统，