A 40 km Fiber－optic Microwave Subcarrier Multiplexing Transmission System for Multi－channel FM－TV

Ａ４０ｋｍＦｉｂｅｒ－ｏｐｔｉｃＭｉｃｒｏｗａｖｅＳｕｂｃａｒｒｉｅｒＭｕｌｔｉｐｌｅｘｉｎｇＴｒａｎｓｍｉｓｓｉｏｎＳｙｓｔｅｍｆｏｒＭｕｌｔｉ－ｃｈａｎｎｅｌＦＭ－ＴＶＺＨＡＮＧＺｈｅｎｇｘｉａｎ；ＬＩＮＺｈｉｙｕａｎ；ＬＩＺｈｉｔａｎｇ；ＸｕＪ...     

Two－Side Electron Beam Pumping System For Hundred－Joule－Level KrF Excimer Laser

Ｔｗｏ－ＳｉｄｅＥｌｅｃｔｒｏｎＢｅａｍＰｕｍｐｉｎｇＳｙｓｔｅｍＦｏｒＨｕｎｄｒｅｄ－Ｊｏｕｌｅ－ＬｅｖｅｌＫｒＦＥｘｃｉｍｅｒＬａｓｅｒ￥ＭＡＷｅｉｙｉ；ＳＨＡＮＹｕｓｈｅｎｇ；ＺＨＯＵＫｕｎｇｏｎｇ；ＷＡＮＧＹｏｕｔｉａｎ；ＺＨＡＮＧＤｏｎｇ；...     

A Two-layer Intrinsically Fuzzy Morphology Image Processor Architecture

ＡＴｗｏ－ｌａｙｅｒＩｎｔｒｉｎｓｉｃａｌｌｙＦｕｚｚｙＭｏｒｐｈｏｌｏｇｙＩｍａｇｅＰｒｏｃｅｓｓｏｒＡｒｃｈｉｔｅｃｔｕｒｅ￥ＳＨＡＯＬａｎ；ＬＩＵＬｉｒｅｎ；ＬＩＧａｕｏｑｉａｎｇ（ＳｈａｎｇｈａｉＩｎｓｔｉｔｕｔｅｏｆＯｐｔｉｃｓａｎｄＦｉｎ...     

A Copper Laser with Flowing Ne-HBr Buffer Gas

ＡＣｏｐｐｅｒＬａｓｅｒｗｉｔｈＦｌｏｗｉｎｇＮｅ－ＨＢｒＢｕｆｆｅｒＧａｓ￥ＪＩＹｉｎｇ；ＬＩＡＮＧＰｅｉｈｕｉ；ＳＨＥＮＱｉｍｉｎ；ＺＨＡＮＧＧｕｉｙａｎ；ＬＩＮＦｕｃｈｅｎｇ（ＳｈａｎｇｈａｉＩｎｓｔｉｔｕｔｅｏｆＯｐｔｉｃｓａｎｄＦｉｎｅＭｅ...     

Tunable Solid-State Laser Using Organic Dye DCM Doped ORMOSIL

ＴｕｎａｂｌｅＳｏｌｉｄ－ＳｔａｔｅＬａｓｅｒＵｓｉｎｇＯｒｇａｎｉｃＤｙｅＤＣＭＤｏｐｅｄＯＲＭＯＳＩＬ￥ＹＥＨｕｉ；ＨＵＷｅｎｔａｏ；ＪＩＡＮＧＺｈｏｎｇｈｏｎｇ（ＳｈａｎｇｈａｉＩｎｓｔｉｔｕｔｅｏｆＯｐｔｉｃｓａｎｄＦｉｎｅＭｅｃｈａｎｉｃｓ...     

Diode-Pumped Monolithic Nd:LMA Laser

Ｄｉｏｄｅ－ＰｕｍｐｅｄＭｏｎｏｌｉｔｈｉｃＮｄ：ＬＭＡＬａｓｅｒ￥ＬＵＪｉａｎｇ；ＨＵＡＮＧＺｈａｏｍｉｎｇ；ＪＩＮＺｈｅｎｈｏｎｇ；ＷＡＮＧＹａｎｇｊｕｎ（ＯｐｔｉｃａｌＦｉｂｅｒＩｎｓｔｉｔｕｔｅ，，ＳｈａｎｇｈａｉＵｎｉｖｅｒｓｉｔｙｏｆＳｃ...     

Single－Mode CW 532nm Output of 1．3W by Internal Frequency Doubling with Ti：MgO：LiNbO_3

Ｓｉｎｇｌｅ－ＭｏｄｅＣＷ５３２ｎｍＯｕｔｐｕｔｏｆ１．３ＷｂｙＩｎｔｅｒｎａｌＦｒｅｑｕｅｎｃｙＤｏｕｂｌｉｎｇｗｉｔｈＴｉ：ＭｇＯ：ＬｉＮｂＯ_３￥ＬＩＪｉａｎ；ＷＵＬｉｎｇ－Ａｎ（ＩｎｓｔｉｔｕｔｅｏｆＰｈｙｓｉｃｓ，ＡｃａｄｅｍｉａＳｉｎｉｃ?..     

Complex-valued Vector-matrix Multiplication Architecture

Ｃｏｍｐｌｅｘ－ｖａｌｕｅｄＶｅｃｔｏｒ－ｍａｔｒｉｘＭｕｌｔｉｐｌｉｃａｔｉｏｎＡｒｃｈｉｔｅｃｔｕｒｅ￥ＺＨＯＵＣｈａｎｇｈｅ；ＬＩＵＬｉｒｅｎ（ＳｈａｎｇｈａｉＩｎｓｔｉｔｕｔｅｏｆＯｐｔｉｃｓａｎｄＦｉｎｅＭｅｃｈａｎｉｃｓ，Ａｃａｄｅｍｉａ...     

Study of Nonlinear Optical Properties of Organic Material Utilizing Two－color Z－scan

ＳｔｕｄｙｏｆＮｏｎｌｉｎｅａｒＯｐｔｉｃａｌＰｒｏｐｅｒｔｉｅｓｏｆＯｒｇａｎｉｃＭａｔｅｒｉａｌＵｔｉｌｉｚｉｎｇＴｗｏ－ｃｏｌｏｒＺ－ｓｃａｎＹＡＮＧＭｉａｏ；ＹＩＮＺｕｘｉｎｇ；ＬＩＦｅｎｇ；ＳＯＮＧＹｉｎｇｌｉｎ；ＬＩＣｈｕｎｆｅｉ（Ｄｅｐ...     

Faraday isolator using permanent magnets

ＦａｒａｄａｙｉｓｏｌａｔｏｒｕｓｉｎｇｐｅｒｍａｎｅｎｔｍａｇｎｅｔｓＳＨＥＮＸｉａｏｈｕａ；ＭＥＮＧＳａｏｘｉａｎ；ＴＩＡＮＬｉ；ＭＡＯＨａｎｆｅｎ；ＹＡＮＧＪｉｎｇｘｉｎ（ＳｈｏｎｇｈａｉＩｎｓｔｉｔｕｔｅｏｆＯｐｔｉｃｓａｎｄＦｉｎｅＭｅｃｈ...     

银薄膜对光学基底表面粗糙度及光散射的影响

为了研究金属银薄膜与光学基底表面粗糙度和光散射的关系,提出了通过对光学薄膜矢量散射公式积分来获得界面粗糙度完全相关模型和完全非相关模型下其表面的总反射散射的方法.理论计算了光学基底上两种模型在不同厚度银膜下的总反射散射和双向反射分布函数.结果表明,当沉积在光学基底上的银薄膜的厚度大于80 nm后,两种模型下计算的银薄膜的表面总反射散射都等于基底的总积分散射,银薄膜能较好地复现出基底的粗糙度轮廓.实验研究表明为了复现基底的粗糙度,银薄膜的最佳厚度应在80~160 nm之间.     

La掺杂浓度对PLZT薄膜红外光学性质的影响

采用溶胶-凝胶法在Pt/Ti/SiO2/Si衬底上制备了不同La掺杂浓度PLZT(x/40/60)薄膜- x射线衍射分析表明制备的PLZT(x/40/60)薄膜是具有单一钙钛矿结构的多晶薄膜- 通过红外椭圆偏振光谱仪测量了波长为2-5—12-6μm范围内PLZT薄膜的椭偏光谱，采用经典色 散模型拟合获得PLZT薄膜的红外光学常数，同时也拟合获得PLZT薄膜的厚度- 随着La掺杂浓 度的增大，折射率逐渐减小- 而消光系数除PLZT(4/40/60)薄膜外，呈现逐渐增大的趋势- 分析表明这些差异主要与PLZ 关键词： PLZT薄膜 红外光学性质 红外椭圆偏振光谱     

化学法制备的HfO2薄膜的激光损伤阈值研究

 采用化学法制备了HfO₂介质膜，研究了热处理、紫外辐照以及Al₂O₃复合对HfO₂介质膜激光损伤阈值的影响。采用红外光谱（FTIR）和X射线衍射仪对薄膜进行了表征，并用输出波长为1.064 μm、脉宽为10 ns的电光调Q激光系统测试薄膜的激光损伤阈值。实验结果表明：采用150 ℃左右的温度对薄膜进行热处理可以提高薄膜的激光损伤阈值，所获得的薄膜的激光损伤阈值高达42.32 J/cm²，比热处理前的激光损伤阈值提高了82%；无机材料Al₂O₃的适量添加能够提高薄膜的激光损伤阈值，其中HfO₂与Al₂O₃的最佳质量配比约为95∶5；另外，对薄膜进行适当的紫外辐照也可改善HfO₂ 薄膜以及HfO₂-Al₂O₃复合薄膜的抗激光损伤性能。紫外辐照对提高HfO₂-Al₂O₃复合薄膜的激光损伤阈值效果尤为显著，辐照40 min后的激光损伤阈值达到44.33 J/cm²，比紫外辐照前的激光损伤阈值提高了90%。     

Y2O3稳定ZrO2薄膜的结构和光学特性

用电子束蒸发法制备出四种不同Y2O3含量的Y2O3稳定ZrO2（YSZ）薄膜,用X射线衍射和透射光谱测定薄膜的结构和光学性能.结果表明：随着Y2O3含量的增加,ZrO2薄膜从单斜相向高温相（四方相和立方相）转变,获得了结构稳定的YSZ薄膜;YSZ薄膜的晶粒尺寸都比ZrO2薄膜的大,但随着Y2O3加入量的增加,晶粒尺寸有减小的趋势,薄膜表面也趋向光滑平整.所有YSZ薄膜的透射谱线都与ZrO2薄膜相似,在可见光和红外光区都有较高的透过率.Y2O3的加入还可以改变薄膜的折射率,在一定范围内可得到所需的任意折射率.     

靶压对磁控溅射GeC薄膜折射率的影响

采用磁控溅射技术,以碳氢气体和氩气为工作气体,在Ge基底上制备了GeC薄膜。研究了靶压对薄膜折射率的影响,发现在较高的靶压下制备的GeC薄膜具有较低的折射率,而在较低的靶压下则得到了高折射率的薄膜。通过控制溅射靶压,制备了折射率在2．5～3．8之间可变的GeC薄膜。利用拉曼光谱研究了GeC薄膜的结构。薄膜样品的硬度测试表明,较低折射率的GeC薄膜具有较高的硬度。     

溅射粒子能量对金属Mo薄膜表面特性的影响

利用原子力显微镜研究了不同溅射离子能量对Mo薄膜表面形貌的影响.利用特殊设计的夹具，在同一真空内完成所有薄膜样品的制备，减少了多次沉积过程对薄膜生长特性的影响 .对原子力显微镜测量得到的表面高度数据进行相关运算，从统计角度定量地研究了不同沉积能量下Mo薄膜表面特性.结果表明，薄膜表面具有典型的分形特征，在相关运算的基础上给出表面的分形维数、水平相关长度、界面宽度等参数.其中，屏栅电压为500V时制备 的薄膜样品与300和700?V时制备的薄膜样品表面的界面宽度及水平相关长度具有倍数差别，但三种溅射电压下薄 关键词： 离子束溅射 钼 薄膜 分形     

Effects of doping concentration on properties of Mn-doped ZnO thin films

This paper reports that the radio frequency magnetron sputtering is used to fabricate ZnO and Mn-doped ZnO thin films on glass substrates at 500~°C. The Mn-doped ZnO thin films present wurtzite structure of ZnO and have a smoother surface, better conductivity but no ferromagnetism. The x-ray photoelectron spectroscopy results show that the binding energy of Mn_2p3 / 2 increases with increasing Mn content slightly, and the state of Mn in the Mn-doped ZnO thin films is divalent. The chemisorbed oxygen in the Mn-doped ZnO thin films increases with increasing Mn doping concentration. The photoluminescence spectra of ZnO and Mn-doped ZnO thin films have a similar ultraviolet emission. The yellow green emissions of 4~wt.% and 10~wt.% Mn-doped thin films are quenched, whereas the yellow green emission occurs because of abundant oxygen vacancies in the Mn-doped ZnO thin films after 20~wt.% Mn doping. Compared with pure ZnO thin film, the bandgap of the Mn-doped ZnO thin films increases with increasing Mn content.     

Stresses and deformation processes in thin films on substrates

The stresses that develop in thin films on substrates can be detrimental to the reliability of thin film electronic devices. In order to design these devices for improved mechanical reliability, an understanding of the origin of these stresses and the controlling deformation processes in thin films is needed. This review begins with a discussion of the basic techniques used for measuring stresses in thin films and for studying the mechanical properties of thin films. The proposed models for the origin of stresses in thin films are then reviewed. Finally, the effects of microstructure and substrate constraint on thin film deformation processes are discussed.     

Deposition of hexagonal boron nitride thin films on silver nanoparticle substrates and surface enhanced infrared absorption

Silver nanoparticle thin films with different average particle diameters are grown on silicon substrates. Boron nitride thin films are then deposited on the silver nanoparticle interlayers by radio frequency （RF） magnetron sputtering. The boron nitride thin films are characterized by Fourier transform infrared spectra. The average particle diameters of silver nanoparticle thin films are 126.6, 78.4, and 178.8 nm. The results show that the sizes of the silver nanoparticles have effects on the intensities of infrared spectra of boron nitride thin films. An enhanced infrared absorption is detected for boron nitride thin film grown on silver nanoparticle thin film. This result is helpful to study the growth mechanism of boron nitride thin film.     

PcNi-VO2复合膜相变光谱特性研究

采用射频磁控溅射的方法在蓝宝石衬底上沉积了高品质的VO2薄膜,并在其上旋涂了酞菁镍[C8H17O]8PcNi薄膜.通过XRD研究了VO2薄膜的微结构.利用红外光谱仪观察了PcNi/VO2复合膜相变前后光学性质的改变,发现PcNi膜在1.5～5.5 μm对VO2膜有增透作用,PcNi/VO2复合膜相对于VO2膜的热色性和相变温度都没有改变.预期PcNi/VO2膜比单一PcNi膜和VO2膜的光限幅能力会更强.