Two-dimensional DFB laser fabricated on dye-doped hybrid zirconia film by soft lithography

A two-dimensional(2D) distributed feedback(DFB) structure is fabricated on dye-doped sol-gel derived hybrid zirconia films by soft lithography.The Q-switched Nd:YAG laser(λ = 532 nm) is used to pump these structures.The lasing emissions of the gain medium doped with Rhodamine 6G(Rh6G) in two perpendicular directions are shown,and the threshold pump energy is measured.     

Multi-wavelength fiber source based on double-pass superfluorescent fiber source and a reflection Mach-Zehnder filter

A spectrum-sliced multi-wavelength fiber source (SS-MWFS) based on double-pass superfluorescent fiber source (SFS) with a reflection Mach-Zehnder filter (RMZF) as the reflected comb filter is demonstrated. With backward pumped configuration, MWFS with 50 wavelength channels of extinction ratio (ER) of 16.7 dB is obtained over the almost total C-band gain region. Total output power of the MWFS is 16.2 mW which shows that a power of about 0.3 mW of per channel is achieved. The SS-MWFS with forward pumped configuration is also discussed for comparing. The backward pumped configuration can provide a larger output power while only a little smaller ER than that of the forward pumped configuration.     

石英玻璃微球吸收光谱上的结构共振

通过CO2激光器熔融不同直径的熔锥光纤以得到相应直径的石英玻璃微球,利用此微球和熔锥光纤,构造了球微腔耦合系统。实验中利用光腰直径为3.1μm的熔锥光纤与直径为143.1μm的石英玻璃微球进行耦合,通过最大分辨力为1pm的可调谐半导体激光器对该耦合系统进行光谱扫描,发现石英玻璃微球的吸收光谱中出现分立的结构共振峰。利用光学微球腔理论讨论了石英玻璃微球吸收光谱中的结构共振,并用米氏散射理论公式对一阶TE模共振峰的位置以及它们的间隔进行了计算,共振峰位置实验结果与理论结果的误差仅为0.03%,表明实验与计算结果相符。     

利用三维构效关系确定互变异构抑制剂的活性构象

HPPD酶抑制剂NTBC存在多种互变异构体,其优势构象受溶液环境影响显著,不同的观测手段确定NT-BC的优势结构存在差异.本文首次采用了三维构效关系CoMFA和CoMSIA对NTBC类似物的5种可能的活性构象进行了研究.根据NTBC类似物以离子为活性构象得到的CoMFA模型具有最佳预测能力,推测NTBC以离子形式与HPPD键合,该结论与文献通过动力学实验预测的结合模式相吻合,这对进一步研究HPPD与NTBC的作用机理以及开发高效抑制剂提供了理论依据.     

在C_(70)固体p-GaAs结构中的甚深深能级

发展了恒温电容瞬态数据处理方法 ,称新方法为恒温电容瞬态时间积谱 (ICTTS) .用ICTTS方法测量分析了C70固体 p GaAs异质结的深能级 ,结果发现在C70 固体中存在两个很深的空穴陷阱 ,H1 和H2 ,它们的能级位置分别为Ev 0 85 6eV和Ev 1 0 37eV     

阻抑动力学光度法测定环境水样中的痕量苯酚

基于在稀硫酸介质中，痕量苯酚能灵敏地阻抑高碘酸氧化苯胺蓝褪色，研究了该阻抑褪色反应的最佳条件及动力学参数，建立了测定痕量苯酚的新方法。该方法的线性范围为0-40.0μg/L，线性回归方程为1g(A1/A2)=0.638c 0.00117，相关系数r=0.9996，检出限为1.2μg/L。该方法简便，灵敏，选择性好，用于环境水样中痕量苯酚的测定，结果准确。     

阻抑动力学光度法测定痕量间二硝基苯

在硫酸介质中,痕量间二硝基苯能灵敏地阻抑Fe3+催化H2O2氧化中性红染料褪色的反应,由此建立了一种测定痕量间二硝基苯的阻抑动力学光度法。采用固定时间法,在λmax=530 nm处,对阻抑体系和非阻抑体系进行光度测定,应用正交试验法确定该阻抑褪色反应的最佳实验条件,并测定了其反应级数。该方法线性范围为0～48μg/L,检出限0.103μg/L,回收率为97.8%～98.9%,测定结果的相对标准偏差为1.5%～2.1%。该方法用于环境水样中间二硝基苯含量的测定,测定结果可靠。     

THE INTERACTION OF Au AND THE Si/SiO2 INTERFACE DEFECT Hit(0.494)

The defects at the Si/SiO₂ interface have been studied by the deep-level transient spectroscopy (DLTS) technique in p-type MOS structures with and without gold diffusion. The experimental results show that the interaction of gold and Si/SiO₂ interface defect,H_it(0.494), results in the formation of a new interface de-fect, Au-H_it(0.445). Just like the interface defect, H_it(0.494), the new interface defect possesses a few interesting properties, for example, when the gate voltage applied across the MOS structure reduces the energy interval between Fermi-level and Si valence band of the Si surface to values smaller than the hole ionization Gibbs free energy of the defect, a sharp DLTS peak is still observable; and the hole apparent activation energy increases with the decrease of the Si surface potential barrier height. These properties can be successfully explained with the transition energy band model of the Si/SiO₂ interface.     

Highly efficient cascaded P-doped Raman fiber laser pumped by Nd:YVO4 solid-state laser

A highly efficient cascaded P-doped Raman fiber laser （RFL） pumped by a 1064-nm continuous wave （CW） Nd：YVO4 solid-state laser is reported. 1.15-W CW output power at 1484 nm is obtained while the input pump power is 4 W, corresponding to the power conversion efficiency of 28.8%. The threshold pump power for the second-order Stokes radiation is 1.13 W. The slope efficiency is as high as 42.6%. The experimental results are in good agreement with theoretical ones. Furthermore, the power instability of the P-doped RFL at 1484 nm in an hour is observed to be less than 5%.