高能、超短脉冲、可调谐激光器用掺镱氟磷酸盐玻璃研究进展

Yb^3 与其它稀土离子相比有最简单的能级结构，这使它具有一些独特的性质，如避免激发态吸收，消除上转换和浓度猝灭等，因此它是高能输出激光器介质的理想掺杂离子。氟磷玻璃综合了氟化物玻璃和磷酸盐玻璃的优点，可降低磷酸盐的声子能量，改善其易吸湿性；提高氟化物玻璃的物理化学性能等，这使它成为稀土掺杂可调谐光纤激光器的很好的掺杂介质。众多研究表明，Yb^3 掺杂氟磷玻璃是一种很有前途的激光工作物质。本文总结了Yb^3 掺杂氟磷玻璃的特点，性质，结构及存在的问题。     

Yb3+掺杂铝氟磷酸盐玻璃的光谱和激光性能

研究了Yb3 掺杂铝氟磷酸盐 (AFP)玻璃的吸收光谱、荧光光谱 ,测量了Yb3 离子的荧光有效线宽 (Δλeff>5 5nm)以及2 F5 2 能级的荧光寿命 (τmax=2ms)及随掺杂浓度的变化 .应用倒易法计算了Yb3 的发射截面 ,其发射截面可达 0 6 6 82 3pm2 ,且激光增益系数τfσemi达 1 2 89ms.pm2 .评估了Yb3 在AFP玻璃中的激光性能 ,发现其具有较理想的激发态最小粒子数 (0 15 )、饱和抽运强度 (8 3kW cm2 )和最小抽运强度 (1 2 4 5kW cm2 )值及良好的热稳定性 .研究结果表明掺Yb3 氟磷酸盐玻璃是实现高功率超短可调谐激光器的理想增益介质 .     

用VB5访问具有用户级安全的Access97数据库

作为Office 97专业版的重要组件,Access 97是开发中小型关系数据库系统的最强大平台之一。在数据库安全方面,Access 97提供了类似网络中使用的方法:设置用户级安全,它要求用户在启动数据库引擎时需确认自己的身份并键入密码;并只能按规定的权限使用数据库中的对象,从而有效地保护了数据库中的敏感数据。 VB5程序员可以通过DAO(数据访问对象)方法使用与驱动Access 97相同的Microsoft Jet数据库引擎V3.5,但可能出于技术和策略上的考虑,VB5并不能象Access 97那样可以创建一个用户级安全的数据库:即它无法创建工作组信息文件.MDW(数据库)。然而,对于一个现存的具有用户级安全的Access数据库,     

用于1．54μm微片激光器的高Er^3＋／Yb^3＋共掺杂的氟铝酸盐玻璃

本文系统制备了980nm半导体崩浦的应用于1．54μm波段微片激光器的高Er^3 ／Yb^3 共掺杂的氟铝酸盐玻璃。通过玻璃的吸收光谱，发射光谱和上转换荧光光谱的测试，对其光学性质、浓度淬灭及其淬灭机制进行了分析和讨论。当玻璃中Er^3 离子掺杂浓度低于10mol％的情况下，浓度淬灭现象较弱，Er^3 ／Yb^3 共掺杂的氟铝酸盐玻璃在由于Er^3 离子^4 I13／2→4^I 15／2跃迁所引起的1．54μm波段的发射强度比Er^3 单掺杂的氟铝酸盐玻璃中的荧光强度要强。在Er^3 离子掺杂浓度高于10mol％的情况下，由于Er^3 与Yb^3 之间的反能量转移过程，Er^3 ／Yb^3 共掺杂的氟铝酸盐玻璃的1．54μm波段的荧光浓度淬灭效应比Er^3 离子单掺杂的情况下明显。在Er^3 离子掺杂浓度小于10mol％的情况下，实验中发现可获得1．54μm波段高发射效率的Er^3 与Yb^3 离子最佳摩尔浓度掺杂比例约为1：1。     

Intense Green Upconversion Luminescence in Er^3＋：Yb^3＋ Codoped Fluorophosphate Glass Ceramic Containing SrTe5O11 Nanocrystals

Er^3＋ ：Yb^3＋ codoped tellurite-fluorophosphate （TFP） glass ceramic exhibits much stronger upconversion luminescence. The intensity of the 540nm green light and 651 nm red light of the TFP glass ceramic is 120 times and 44 times stronger than that of the fluorophospahte （FP） glass, respectively. XRD analysis shows that the nanocrystal in TFP glass ceramic is SrTe5O11. TFP glass ceramic also displays much higher upconversion fluorescence lifetime and crystallization stability. The narrow and strong peak at 540nm is very ideal for practical upconversion luminescence realization. This work is a new trial for exploring non-PbF2 involved nanocrystal upconversion glass ceramics.     

光折变晶体全息存储的串扰噪声

对页间和页内串扰噪声进行了理论分析。通过实验研究串扰噪声。实验结果表明，在进行大规模全息存储过程中复用角度间隔△θ〉△Θ时，读出后的图像能够完全分辨，图像像元越小页内串扰噪声越大。     

最大熵方法在准连续波体制中的实现

本文分析了最大熵方法的特点和准连续波体制原理,提出了用于雷达接收机系统的最大熵谱预测外推算法的选择依据,设计实现了以TMS320C31为主芯片的核心外推运算单元,完成了对最大熵谱预测外推电路的实时监控。信号传输速率达到40Mb/s,当定义外推算法为8阶时,数据吞吐量达到1Mb/s。本文所做工作对准连续波雷达走向实际应用具有较大意义。     

A polarized micro-Raman study of a 0.65PbMg1/3Nb2/3O3 - 0.35PbTiO3 single crystal

Polarized micro-Raman spectra of a 0.65PbMg_1/3Nb_2/3O₃-0.35PbTiO₃ (0.65PMN-0.35PT) single crystal poled in the [001] direction are obtained in a wide frequency range (50-2000 cm^-1) at different temperatures. The best fit to the Raman spectrum at 77 K is achieved using 17 Lorenzians to convolute into it, and this is proved to be a reasonable fit. According to the group theory and selection rules of overtone and combinational modes, apart from the seven Raman modes that are from first-order Raman scattering, the remaining ones are attributed to being from second-order Raman scattering. A comparison between the experimental results and theoretical predictions shows that they are in satisfactory agreement with each other. Our results indicate that at 77 K the sample belongs to the rhombohedral symmetry with the C_3v⁵ (R3m) space group (Z=1). In our study, on heating, the 0.65PMN-0.35PT single crystal undergoes a rhombohedral to tetragonal to cubic phase transition sequence. The two phase transitions occur at 340 and 440 K, which correspond to the disappearance of the soft mode near 106 cm^-1 recorded in VV polarization and the vanishing of the band around 780 cm^-1 in VH polarization, respectively.     

A polarized micro-Raman study of a 0.65PbMg1/3Nb2/303-0.35PbTi03 single crystal

Polarized micro-Raman spectra of a 0.65PbMg_1/3Nb_2/3O₃-0.35PbTiO₃ （0.65PMN-0.35PT） single crystal poled in the [001] direction are obtained in a wide frequency range （50-2000 cm 1） at different temperatures.The best fit to the Raman spectrum at 77 K is achieved using 17 Lorenzians to convolute into it,and this is proved to be a reasonable fit.According to the group theory and selection rules of overtone and combinational modes,apart from the seven Raman modes that are from first-order Raman scattering,the remaining ones are attributed to being from second-order Raman scattering.A comparison between the experimental results and theoretical predictions shows that they are in satisfactory agreement with each other.Our results indicate that at 77 K the sample belongs to the rhombohedral symmetry with the C 5 3v （R3m） space group （Z=1）.In our study,on heating,the 0.65PMN-0.35PT single crystal undergoes a rhombohedral → tetragonal → cubic phase transition sequence.The two phase transitions occur at 340 and 440 K,which correspond to the disappearance of the soft mode near 106 cm 1 recorded in VV polarization and the vanishing of the band around 780 cm 1 in VH polarization,respectively.     

一种适用于混响环境的麦克风阵列语音增强方法

在小型视频会议系统中,影响语音处理系统性能的主要因素是房间混响效应.现有语音增强方法大都采用加性噪声模型,没有考虑混响;而基于倒谱的语音去混响方法大多计算复杂.为此,本文给出了一种改进的麦克风阵列倒谱域语音去混响方法.该方法首先计算含噪语音倒谱域的最小相位分量,并对其进行波束形成,再进行低通滤波;然后利用人耳对相位信息的不敏感性,采用含噪语音的相位来合成增强后的语音信号,从而有效地降低了运算量.仿真结果表明,该方法在混响环境下能有效地改善语音质量.