非谐振腔型KTP光参变振荡器

研究了双晶体走离补偿、非谐振腔型KTP光参变振荡器，利用一套膜片实现了KTP相位匹配所允许的全波段调谐，信号光调谐范围0.698μm-1.026μm，闲频光调谐范围1.105μm-2.237μm。5倍阈值处，信号光840nm最高输出能量53mJ，能量转换效率25.8%，量子转换效率40％，闲频光的量子郊率也达到32％。     

PEO／PBHE共混体系X射线散射研究

在聚环氧乙烷(PEO)/聚双酚A羟基醚(PBHE)共混体系中PEO是一个强质子受体,而PBHE是一个强质子给体,两者极易形成氢键,十分有利于形成互容对。笔者研究了PEO/PBHE共混体系的相容性,等温及非等温结晶动力学,本文根据Vonk提出的一维电子密度相关函数,分析了PEO/PBHE的SAXS现象,求得了共混体系的结晶度,片晶层厚度,过渡层厚度及长周期等结构参数。     

导热增强聚乙二醇相变复合材料的制备及其性能

本文以聚乙二醇(PEG)为相变材料,通过添加不同的无机填料,采用熔融共混浇筑方式制备了导热增强型相变复合材料。 通过扫描电子显微镜(SEM)、热常数分析仪、差示扫描量热仪(DSC)、红外热成像和热重分析仪研究了所制备复合材料的微观结构、导热性能与相变过程。 研究结果表明,相比于碳酸钙和氧化铝,在相同添加含量下,氮化硼(BN)可有效提高PEG的导热系数,当BN质量分数为40%时,导热系数可达到3.40 W/(m·K);当填料添加量相同时,片状BN和不规则纳米碳酸钙(CaCO₃)比球形氧化铝(Al₂O₃)对PEG具有更加优良的定型效果,在相变过程中,能够更加有效阻隔PEG的流动,保持复合材料的形状稳定性。     

高质量CdSe单晶生长及其OPO性能研究

本文利用有籽晶的HPVGF法生长了尺寸为φb54 mm× 25 mm的高质量CdSe单晶,晶体为纤锌矿结构,(002)和(110)面的XRD摇摆曲线半高宽分别为54.4"和45.6".使用红外显微镜和扫描电镜-能谱分析仪对晶体内部的夹杂相进行测试,表明晶体内部存在小尺寸富Se夹杂相.CdSe晶片在2.5～20 μm范围内的透过率高于68;,平均吸收系数为0.037 cm-1.制备出尺寸为10mm×12 mm×50mm且满足第Ⅱ类相位匹配条件的CdSe晶柱,在重频1 kHz,波长2.09 μm的Ho∶ YAG调Q泵浦源激励下,实现了中心波长为11.47 μm,线宽为33.2 nm的激光输出,最大输出功率为389 mW.     

VEGA: visual comparison of phylogenetic trees for evolutionary genome analysis (ChinaVis 2019)

In the field of evolutionary genome analysis, biologists seek to identify important genes or chromosome regions by comparing phylogenetic trees and analyzing the mutation at which locus might affect phenotypic traits. Unfortunately, the tree comparison and accompanying analysis are often performed manually. In this paper, we characterize the workflow of evolutionary genome analysis and present a task analysis for the fundamental questions asked by biologists during the analysis procedure. We propose two algorithms to enable quantitative tree comparison. One is to measure the differences between corresponding leaf nodes on two trees, and the other is to compute the classification inconsistency of each leaf node by comparing tree structure with a given biological classification. Configuring with the obtained difference and inconsistency, we present a visual analysis system, visual comparison of phylogenetic trees for evolutionary genome analysis, which not only enables biologists to intuitively explore trees but also identify locus which affects their traits by comparing SNP variants of selected leaf nodes. We conclude with case studies from two biologists who used our system to augment their previous manual analysis workflow and demonstrate that our system can reveal more insight.     

有机物/硅杂化太阳能电池的研究进展

有机/无机杂化太阳能电池既可以兼容无机材料的高稳定性, 高载流子迁移率和成熟的制备工艺, 又可以利用有机材料分子结构的可塑性, 调节光谱吸收以及光学带隙, 以及简便的溶液制作过程, 具有取得高效率低成本太阳能电池的巨大潜力. 硅和有机物在低温下形成的异质结光伏电池吸引了广泛的研究, 目前最高光电转换效率已经达到13.8%. 而采用硅纳米线等纳米结构之后使在几十微米的低纯硅上制备高效太阳能电池成为可能, 柔性硅基底的杂化太阳能电池效率已经超过12%. 本文首先介绍了硅基杂化太阳能电池的结构、工作机理和使用的有机材料, 按硅的结构分为平面硅基和微纳结构硅基杂化太阳能电池, 重点概述了该类电池最近几年的发展状况, 分析了硅的结构、有机材料和制备工艺对器件性能的影响. 最后对众多研究方法进行了归纳总结, 对存在的问题和解决策略提出了展望.     

La15Fe77B8型储氢合金的结构和电化学性能

研究了快淬和退火态La15Fe77B8型储氢合金的组织结构和电化学性能。应用中频感应熔炼-快淬方法制备了La15Fe77B8型储氢合金,其组成为La15Fe2Ni72Mn7B2Al2。结构分析表明:快淬La15Fe2Ni72Mn7B2Al2合金为多相结构,包括LaNi5相、La3Ni13B2相和(Fe,Ni)相,快淬合金经1223 K保温3 h,然后在873 K保温3 h退火处理后,LaNi5相增加,La3Ni13B2相几乎消失,(Fe,Ni)相增加且形态变大。电化学测试表明,退火合金的最大容量(307 mAh.g-1)略小于快淬合金(309 mAh.g-1),而循环稳定性有所改善。退火合金电极的倍率放电能力(HRD)低于快淬合金,原因在于交换电流密度(I0)及氢在合金中的扩散系数(D)降低。快淬和退火合金电极在低温233 K时均能放出55%的容量。     

High-Power in-Band Pumped a-Cut Ho:Yap Laser

We report the continuous wave and acousto-optically Q-switched operation of an in-pumped a-cut Ho:YAP laser at room temperature. We obtained a continuous-wave output power of 17.2 W at 2118 nm under an absorbed pump power of 29.8 W, corresponding to a slope efficiency of 63.2 %. For the Q-switched mode, we achieved a maximum pulse energy of about 1.7 mJ and a minimum pulse width of 24 ns at a repetition rate of 10 kHz, resulting in a peak power of 70.8 kW.     

A periodically poled LiNbO3 optical parametric generator in wavelength conversion from 2 to 3.88-4.34 μm

A periodically poled lithium niobate (PPLN) optical parametric generator (OPG) pumped by a laser diode (LD)-pumped Q-switched Tm,Ho:GdVO4 laser operated at 2.048 μm with pump pulse of 25 ns and repetition rate of 10 kHz is reported.