高功率固体激光近场强度功率谱密度特性分析

高功率固体激光驱动器的负载能力已经成为限制驱动器发展的瓶颈问题,负载能力研究的主要是激光束近场和光学元件的相互作用过程。采用功率谱密度(Power spectral density,PSD)方法分析了多程放大构型高功率固体激光驱动器实验输出近场强度的频谱在激光强度提升过程中的演变规律,分析了引起近场强度调制的主要因素。结果表明,高强度下,激光驱动器的输出近场存在明显的频谱特征,二维功率谱密度近似满足各向同性,近场调制主要源于小尺度自聚焦效应,PSD曲线显示获得增长的频率主要是各级空间滤波器截止频率所限定的频段。     

Realization of MMI Power Splitter by UV-light Imprinting Technique Using Hybrid Sol-Gel SiO2 Materials

An efficient fabrication scheme of buried ridge waveguide devices is demonstrated by UV-light imprinting technique using organic-inorganic hybrid sol-gel Zr-doped SiO2 materials. The refractive indices of a guiding layer and a cladding layer for the buried ridge waveguide structure are 1.537 and 1.492 measured at 1550nm, respectively. The tested results show more circular mode profiles due to existence of the cladding layer. A buried ridge single-mode waveguide operating at 1550 nm has a low propagation loss （0.088 dB/cm） and the 1× 2 MMI power splitter exhibits uniform outputs, with a very iow splitting loss of 0.029 dB at 1549nm.     

延长速调管使用寿命的方法

描述了一种延长EPR波谱仪中速调管使用寿命的方法.根据这种方法,只要正确地调谐微波桥的工作状态和适当地调整功率电平器的功率校正电平.即使对于已经严重老化的速调管仍然可以继续使用一段时间,维持仪器的正常运行.     

Comparison of Nd:YAG Ceramic Laser Pumped at 885nm and 808nm

Laser performance of 1064 nm domestic Nd：YAG ceramic lasers for 885 nm direct pumping and 808 nm traditional pumping are compared. Higher slope efficiency of 34% and maximum output power of 16.5 W are obtained for the 885nm pump with a 6ram length 1 at.% Nd：YAG ceramic. The advantages for 885nm direct pumping are discussed in detail. This pumping scheme for highly doping a Nd：YAG ceramic laser is considered as an available way to generate high power and good beam quality simultaneously.     

All-Solid-State Nd:YAG Laser Operating at 1064nm and 1319nm under 885nm Thermally Boosted Pumping

We report a high-effciency Nd：YAG laser operating at 1064 nm and 1319nm, respectively, thermally boosted pumped by an all-solid-state Q-switched Ti：sapphire laser at 885 nm. The maximum outputs of 825.4 m W and 459.4mW, at 1064nm and 1319nm respectively, are obtained in a 8-ram-thick 1.1 at.% Nd：YAG crystal with 2.1 W of incident pump power at 885nm, leading to a high slope efficiency with respect to the absorbed pump power of 68.5% and 42.0%. Comparative results obtained by the traditional pumping at 808nm are presented, showing that the slope efficiency and the threshold with respect to the absorbed pump power at 1064nm under the 885nm pumping are 12.2% higher and 7.3% lower than those of 808rim pumping. At 1319nm, the slope efficiency and the threshold with respect to the absorbed pump power under 885nm pumping are 9.9% higher and 3.5% lower than those of 808 nm pumping. The heat generation operating at 1064 nm and 1319 nm is reduced by 19.8% and 11.1%, respectively.     

非自持和非麦氏分布情况下托卡马克堆芯等离子体功率平衡

本文给出一组托卡马克堆芯等离子体功率平衡方程,它描述了在非自持和非麦氏分布情况下等离子体功率平衡的问题,计算结果表明。在现实可行的聚变堆工程和相应的等离子体参数情况下,堆芯中每秒可产生聚变中子PN大于10~19。     

溅射功率对多层膜质量的影响

用磁控溅射技术制备薄膜，用X射线衍射研究在基片和靶间距离固定的情况下不同的溅射功率对薄膜结构的影响。结果表明：过低的溅射功率下淀积的薄膜有畸变的X射线衍射特征峰，特征峰强度小，半峰全宽大。而比较高溅射功率得到的薄膜有比较尖锐的X射线衍射特征峰，强度高和半峰全宽非常窄。研究表明，X射线衍射特征峰强度小和半峰全宽大的薄膜结构疏松，而强度高和半峰全宽非常窄的薄膜结构致密。     

自聚焦激光束光束质量评价的功率谱密度方法

在高功率激光系统中，介质的非线性折射率引起的小尺度自聚焦效应将会带来对光束相位和强度分布的影响，增加光学元件遭受成丝破坏的风险。产生光束小尺度纹波调制的机制分为两类：振幅和位相调制。振幅调制引起的光束自聚焦是造成介质损伤的主要因素。根据小信号的Bespalov-Talanov理论，只有特定空间频率(或称为模式)的调制具有最快的增长速度，其增长幅度可以用B积分参数来描述。目前，有关光束的自聚焦成丝已经引起了激光器研制人员的重视。     

磁逆多光子非线性Compton散射的谱功率

相对论电子在强磁场中的磁逆Compton散射是一种重要的γ射线辐射机制。虽然对该问题的研究已有二十多年的历史，但对磁逆多光子非线性Compton散射谱功率的研究尚未见报道。本文采用电子与光子非弹性碰撞模型，首次给出了磁逆多光子非线性Compton散射的谱功率。     

HIRFL高频腔体功率耦合匹配实验研究

 介绍了HIRFL主加速器SSC高频腔体功率馈入耦合匹配系统的研究，实验结果表明，通过改变耦合环角度可更好地实现高频腔体和高频发射机之间的匹配，提高了高频腔体电压和高频发射机的工作效率。