飞秒脉冲激光器腔镜二、三阶色散的理论研究

详细研究了飞秒脉冲激光腔镜的结构参数及光束入射角对其二、三阶色散的影响。得出了反射单一定时，二阶色散和三阶色出量随着膜料折射率比值和镀膜层数的增加而变大，当这两个参量分别超过１．６７和２５层时，三阶色散开始振荡．另外发现光束入射均对三阶色散的影响比二阶色散明显。     

二维TLM网格色散特性的数值模拟

用数值模拟方法研究了二维TLM网格的色散特性对传播高斯脉冲波形的影响，同时通过模拟得到波在网格中的传播速度。数值实验表明．色散对高斯脉冲的幅度和前沿都会产生影响，表现为幅度随传播距离的增加而减小，而前沿则变得比后沿陡，且在△l／λ以较大时，例如△l／λ=0．1，脉冲前沿出现振荡现象，振荡的幅度随传播距离的增加而加大。当△l／λ=0．1时，脉冲形状几乎没有变化。数值实验得到的波在网格中的传播速度，与理论计算公式所得传播速度相吻合，其吻合的程度随△l／λ=0．1的减小而增加。     

萘醌并噻唑系化合物三阶非线性光学性质的研究

用三维简并四波混频（ＤＦＷＭ）研究了五种萘醌并噻唑化合物的三阶非线性光学性质。实验测得样品溶液的三阶非线性极化率｜χ（３）Ｓ｜４．３×１０－１３ｅｓｕ，分子的三阶非线性超极化率γＳ４．４×１０－３１ｅｓｕ。分析了分子结构对三阶非线性光学性质的影响。     

激光V型腔参量对输出性能的影响

在激光腔型设计时，为了使激光具有良好的输出性能，需要找出谐振腔参量对激光输出性能的影响规律。结合V型折叠腔的图解分析法和多元件光学谐振腔的等价腔分析法，将折叠腔近似等价后，对等价的共轴球面空腔的稳定性和输出光束质量进行理论求解分析，找到了V型折叠腔参量和激光输出性能的内在联系。通过计算给定的条件可知，当折叠角=0.15时，总腔长L的理想取值范围为（70，80）mm，最佳取值为75 mm，端面镜曲率半径R1、R2的允许变化范围为（60，75）mm，折叠镜曲率半径R3的最小取值为45 mm，随着左（右）侧子腔g-参数积增大，右（左）侧端面镜上的基模光斑半径和远场发散角增大。上述等价腔分析法和结论对激光腔型优化设计提供了重要的理论依据。     

湍流强度对激光大气传输及其自适应光学校正的影响

利用激光大气传输及其相位校正四维程序，计算了不同的发射和传输条件对平台聚焦光束水平大气传输及其自适应光学校正的影响。结果表明：自适应光学系统开环时，在弱湍流效应条件下，以D／r0为特征参量可以很好地表征湍流效应的强弱，SR值满足关系式SR=exp[-0．2（D／r0）^2]，不考虑系统像差时，光束质量因子满足关系式β2=1＋1．2（D／r0）^2；随着湍流强度或传输距离的增加，要考虑闪烁效应和相位不连续性对光束质量的影响，以D／r0为特征参量就不足以表征湍流效应的强弱。另外，对于不同的发射和传输条件，自适应光学系统对激光大气传输的校正范围是不同的，且存在一阈值，条件不同其阈值是不同的。     

基于宽禁带氮化物的微腔光频梳进展（特邀）

微腔光频梳在光谱测量、微波光子学、光学原子钟和相干光通信等领域具有重要的应用。宽禁带氮化物半导体材料,如氮化铝（AlN）和氮化镓（GaN）等属于非中心对称晶体,具有二阶和三阶光学非线性系数,宽带的透明窗口以及与蓝宝石衬底较高的折射率差,使其成为研究非线性光子器件的理想平台。文中介绍了氮化物微腔的特性,同时对基于氮化物微腔光梳的相关研究进展,包括AlN微腔中的宽谱光频梳产生和光学参量振荡、GaN微腔中的孤子光频梳产生等进行了介绍和展望。     

有核细胞Mie相函数的计算与分析

研究光在生物组织中的传输过程时需要更精确的散射相函数,这就需要研究细胞核对相函数的影响。基于几何散射逼近理论修正了单一分散系有核细胞的Mie相函数、不对称因子g和二阶参量γ;分析了有核细胞形态及光学参量对Mie相函数角分布和Airy峰数的影响;对g和γ随入射光波长、细胞尺寸、核质比和折射率的变化规律进行了数值模拟。结果表明:Mie相函数分布、Airy峰数、g和γ不仅与细胞的大小有关,而且与细胞核占比及折射率有关,不能忽略细胞内部光学结构的影响。与HG相函数相比,Mie相函数能够描述侧后向散射特征,更准确地计算g和γ,为研究细胞的免标记识别方法以及激光在生物组织中的传输特性提供了进一步的理论支持。     

一种新的双偶氮化合物的三阶非线性光学性能

合成了一种新的双偶氮化合物2,6-双[(2,4-二羟基苯基)偶氮]蒽醌,用IR,1 H NMR和元素分析表征了其结构.采用飞秒激光,运用简并四波混频法,研究了化合物在非共振状态下的三阶非线性光学性能.它的三阶非线性光学极化率χ(3)为3.37×10-13 esu,非线性折射率n2为6.21×10-12 esu,分子二阶超极化率γ为4.02×10-31 esu,响应时间τ为101 fs.分析了化合物的分子结构对三阶非线性光学性能的影响.增长共轭链,形成供吸供构型,增大取代基的吸或供电子能力等因素有利于获得较大的三阶非线性光学性能.     

非柯尔莫哥诺夫湍流对部分相干双曲余弦高斯光束扩展的影响

基于非柯尔莫哥诺夫湍流模型,本文给出了部分相干双曲余弦高斯光束通过湍流传输的二阶矩束宽和相对束宽解析式,并研究了湍流参数(广义指数α、内尺度l0、外尺度L0)和光束参数(离心参数δ、相干参数β)对光束扩展的影响。研究表明:束宽随α的增大而先增大后减小,且在α=3.11处存在光束扩展极大值;束宽随l0的增大而减小,随L0的增大而略微增大(仅当α3.7时)。另外,束宽随δ的增大及β的减小而增大,但当δ越大和β越小时,光束扩展受湍流的影响则越小。     

双曲余弦高斯光束在非Kolmogorov湍流中的湍流距离

为了研究双曲余弦高斯光束在非Kolmogorov湍流中的扩展,采用广义惠更斯-菲涅耳原理,推导出部分相干双曲余弦高斯光束在非Kolmogorov湍流中的湍流距离zt的解析表达式。对湍流参量(广义指数、内尺度l0、外尺度L0)和光束参量(相干参量、离心参量)对湍流距离的影响进行了理论分析。结果表明,zt随的增大而先减小后增大,且在=3.11处存在zt极小值;zt随l0和的增大而增大,随L0(仅当3.64时)和的增大而减小。这一结果对双曲余弦高斯光束在实际湍流中传输的相关应用是有帮助的。     

Development of the readout system for waveguide multilayer optical card

Waveguide multilayer optical card （WMOC） is a novel storage device of three-dimensional optical information. An advanced readout system fitting for the WMOC is introduced in this paper. The hardware mainly consists of the light source for reading, WMOC, motorized stages addressing unit, microscope imaging unit, CCD detecting unit and PC controlling ＆ processing unit. The movement of the precision motorized stage is controlled by the computer through Visual Basic （VB） language in software. A control panel is also designed to get the layer address and the page address through which the position of the motorized stages can be changed. The WMOC readout system is easy to manage and the readout result is directly displayed on computer monitor.     

Nanoimprint Lithography -A Next Generation High Volume Lithography Technique

IntroductionNanoimprint Lithography is a well-acknowl-edged low cost, high resolution, large area pattern-ing process. It includes the most promising methods,high-pressure hot embossing lithography (HEL) [2],UV-cured imprinting (UV-NIL) [3] and micro contactprinting (m-CP, MCP) [4]. Curing of the imprintedstructures is either done by subsequent UV-lightexposure in the case of UV-NIL or by cooling downbelow the glass transition temperature of the ther-moplastic material in case of HEL…     

Collinear phase-matching study of terahertz-wave generation via difference frequency mixed in GaAs and Inp

The collinearly phase-matching condition of terahertz-wave generation via difference frequency mixed in GaAs and InP is theoretically studied. In collinear phase-matching, the optimum phase-matching wave hands of these two crystals are calculated. The optimum phase-matching wave bands in GaAs and lnP are 0.95-1.38μm and 0.7-0.96μm respectively. The influence of the wavelength choice of the pump wave on the coherent length in THz-wave tuning is also discussed. The influence of the temperature alteration on the phase-matching and the temperature tuning properties in GaAs crystal are calculated and analyzed. It can serve for the following experiments as a theoretical evidence and a reference as well.     

Effects of the alloy compositions on the phonon-polaritons in ternary mixed crystals

Composition dependence of bulk and surface phonon-polaritons in ternary mixed crystals are studied in the framework of the modified random-element-isodisplacement model and the Bom-Huang approximation. The numerical results for Several Ⅱ - Ⅵ and Ⅲ- Ⅴ compound systems are performed, and the polariton frequencies as functions of the compositions for ternary mixed crystals AlxGa1-xAs, GaPxAS1-x, ZnSxSe1-x, GaAsxSb1-x, GaxIn1-xP, and ZnxCd1-xS as examples are given and discussed. The results show that the dependence of the energies of two branches of bulk phonon-polaritons which have phonon-like characteristics, and surface phonon-polaritons on the compositions of ternary mixed crystals are nonlinear and different from those of the corresponding binary systems.     

Influence of PVK ： NPB hole transporting layer on the characteristics of organic light-emitting devices

A doping system consisting of NPB and PVK is employed as a composite hole transporting layer （CHTL）. By adjusting the component ratio of the doping system, a series of devices with different concentration proportion of PVK ： NPB are constracted. The result shows that doping concentration of NPB enhances the competence of hole transporting ability, and modifies the recombination region of charge as well as affects the surface morphology of doped film. Optimum device with a maximum brightness of 7852 cd/m^2 and a power efficiency of 1.75 lm/W has been obtained by choosing a concentration proportion of PVK ： NPB at 1：3.     

New insert layer structure OLEDs

An insert layer structure organic electroluminescent device（OLED） based on a new luminescent material （Zn（salen）） is fabricated. The configuration of the device is ITO/CuPc/NPD/Zn（salen）/Liq/LiF/A1/CuPc/NPD/Zn（salen）/Liq/LiF/A1. Effective insert electrode layers comprising LiF（1nm）/Al（5 nm） are used as a single semitransparent mirror, and bilayer cathode LiF（1 nm）/A1（100 nm） is used as a reflecting mirror. The two mirrors form a Fabry-Perot microcavity and two emissive units. The maximum brightness and luminous efficiency reach 674 cd/m^2 and 2.652 cd/A, respectively, which are 2.1 and 3.7 times higher than the conventional device, respectively. The superior brightness and luminous efficiency over conventional single-unit devices are attributed to microcavity effect.     

Analysis of error performance on Turbo coded FDPIM

Due to variable symbol length of digital pulse interval modulation（DPIM）, it is difficult to analyze the error performances of Turbo coded DPIM. To solve this problem, a fixed-length digital pulse interval modulation（FDPIM） method is provided. The FDPIM modulation structure is introduced. The packet error rates of uncoded FDPIM are analyzed and compared with that of DPIM. Bit error rates of Turbo coded FDPIM are simulated based on three kinds of analytical models under weak turbulence channel. The results show that packet error rate of uncoded FDPIM is inferior to that of uncoded DPIM. However, FDPIM is easy to be implemented and easy to be combined, with Turbo code for soft-decision because of its fixed length. Besides, the introduction of Turbo code in this modulation can decrease the average power about 10 dBm, which means that it can improve the error performance of the system effectively.     

A method for calculating the center position of collimated light

It is a key problem to accurately calculate beam spots＇ center of measuring the warp by using a collimated laser. A new method, named double geometrical center method （DGCM）, is put forward for the first time. In this method, a plane wave perpendicularly irradiates an aperture stop, and a charge couple device （CCD） is employed to receive the diffraction-beam spots, then the geometrical centers of the fast and the second diffraction-beam spots are calculated respectively, and their mean value is regarded as the center of datum beam. In face of such adverse instances as laser intension distributing defectively, part of the image being saturated, this method can still work well. What＇s more, this method can detect whether an unacceptable error exits in the courses of image receiving, processing and calculating. The experimental results indicate the precision of this method is high.     

Preparation and Characterization of TaN ALD Precursors

High purity organic-tantalum precursors for thin film ALD TaN were synthesized and characterized.Vapor pressure and thermal stability of these precursors were studied.From the vapor pressure analysis,it was found that TBTEMT has a higher vapor pressure than any other published liquid TaN precursor,including TBTDET,TAITMATA,and IPTDET.Thermal stability of the alkyl groups on the precursors was investigated using a 1H NMR technique.The results indicated that the tertbutylimino group is the most stable group on TBTDET and TBTEMT as compared to the dialkylamido groups.Thermal stability of TaN precursors decreased in the following order:TBTDET ＞ PDMAT ＞ TBTEMT.In conclusion,precursor vapor pressure and thermal stability were tuned by making slight variations in the ligand sphere around the metal center.     

Curved crystal spectrometer for the measurement of X-ray lines from laser-produced plasmas

In order to diagnose the laser-produced plasmas, a focusing curved crystal spectrometer has been developed for measuring the X-ray lines radiated from a laser-produced plasmas. The design is based on the fact that the ray emitted from a source located at one focus of an ellipse will converge on the other focus by the reflection of the elliptical surface. The focal length and the eccentricity of the ellipse are 1350 mm and 0.9586, respectively. The spectrometer can be used to measure the X- ray lines in the wavelength range of 0.2-0.37 nm, and a LiF crystal （200） （2d = 0.4027 nm） is used as dispersive element covering Bragg angle from 30° to 67.5°. The spectrometer was tested on Shengnang- Ⅱ which can deliver laser energy of 60-80 J/pulse and the laser wavelength is 0.35 μm. Photographs of spectra including the 1 s2p ^1P1-1s^2 ^1S0 resonance line（w）, the 1s2p ^3P2-1s^2 1S0 magnetic quadrupole line（x）, the 1s2p ^3P1-1 s^2 ^1S0 intercombination lines（y）, the 1 s2p ^3S~1-1 s^2 ^1S0 forbidden line（z） in helium-like Ti Ⅹ Ⅺ and the 1 s2s2p ^2P3/2-1 s622s ^2S1/2 line（q） in lithium-like Ti Ⅹ Ⅹhave been recorded with a X-ray CCD camera. The experimental result shows that the wavelength resolution（λ/△ 2） is above 1000 and the elliptical crystal spectrometer is suitable for X-ray spectroscopy.