亚微米直径光纤的非线性特性研究

用电磁场的严格解分析了亚微米直径光纤的非线性系数,发现光纤直径在700 nm左右（亚微米量级）非线性系数较大,喇曼阈值较小,喇曼增益谱线较多;受激喇曼散射特性的分析表明,由于直径小,光纤在较小的泵浦光功率作用下能量密度就很大,因此很容易观察到受激喇曼散射.实验结果表明,理论分析与实验结果吻合得很好.     

高效率激光二极管泵浦100 Hz 3.5 J Nd∶YAG MOPA激光器

研制了结构简单、高效率激光二极管泵浦Nd∶YAGM0PA激光器.振荡级输出单脉冲能量1.13 J,重复频率为100HZ.MOPA系统输出最大单脉冲能量2.35 J,光-光转换效率为39%.实验结果和理论计算符合较好.     

常温直接沉淀法制备ZnO纳米棒

在常温下, 以PEG-400(聚乙二醇400)为表面活性剂, 采用直接沉淀法合成了ZnO纳米棒. 产物用XRD, TEM, SAED和 HRTEM等进行了表征. 结果表明, 所得ZnO为一维的纳米棒, 属于六方纤维矿的单晶结构. ZnO纳米棒的直径在20~40 nm之间, 长度在300~800 nm范围. (0001)面为ZnO纳米棒的生长方向. 讨论了ZnO相的生成和ZnO纳米棒的形成机理以及PEG-400在其形成过程中的作用.     

Hydrothermal Synthesis of Nanorods and Nanowires of Mg/Al Layered Double Hydroxides

Layered double hydroxides (LDHs) are a class of synthetic anion clays, characterized by the formula[MⅡ1-xMⅢx (OH)2]x (An- )x/n·yH2O (where M =metal and A = anion, usually carbonate)[1-3]. A large number of LDHs with a wide variety of M Ⅱ-M Ⅲ cation pairs including M Ⅰ-M Ⅲ ( e. g. , Li-Al ) and M Ⅱ-MⅣ( e. g. , Co-Ti) have been reported. Thus the identities of the cations(MⅠ , MⅡ , MⅢ and MⅣ) and the interlayer anion (An-) together with the value of the stoichiometric coefficient (x) may vary widely, giving rise to a large class of isostructural materials.     

亚微米分子筛粒径与性能的关联研究

对实验室合成的不同粒径的NaY分子筛进行了性能研究,表明比表面积、酸量随着粒径的减小而增加,粒径太小的分子筛其稳定性、活性低,不能满足FCC催化剂的使用要求,应用于FCC催化剂的分子筛合适粒径为500nm～800nm.     

Linear and nonlinear optical properties of ZnO nanorod arrays

Polarization-dependent linear absorption, second-harmonic generation （SHG） and 3rd-order nonlinearities of wellaligned ZnO nanorod arrays have been investigated with ps pulses. The depressed spectral width and the enhanced intensity of reflective SHG along the long axis of ZnO nanorods were observed by using p-polarized pulses, which is explained by the optical confinements. The nonlinear absorption coefficient measured with s-polarization reached the maximum 4.0×10^4cm/GW at the wavelength -750nm, which revealed a large two-photon resonance absorption attributed to the quantum confined exciton when the polarization is vertical to the long axis of ZnO nanorod.     

Growth of β-Ga2O3 nanorods by ammoniating Ga2O3/V thin films on Si substrate

This paper reports that/3-Ga2O3 nanorods have been synthesized by ammoniating Ga2O3 films on a V middle layer deposited on Si（111） substrates. The synthesized nanorods were confirmed as monoclinic Ga2O3 by x-ray diffraction,Fourier transform infrared spectra. Scanning electron microscopy and transmission electron microscopy reveal that the grown β-Ga2O3 nanorods have a smooth and clean surface with diameters ranging from 100 nm to 200 nm and lengths typically up to 2μm. High resolution TEM and selected-area electron diffraction shows that the nanorods are pure monoclinic Ga2O3 single crystal. The photoluminescence spectrum indicates that the Ga2O3 nanorods have a good emission property. The growth mechanism is discussed briefly.     

二极管泵浦Nd:YAG棒双通放大器技术

二极管泵浦NdYAG棒双通放大器采用两个峰值功率6.5 kW激光泵浦模块作为泵浦源.每个激光泵浦模块由81个二极管激光器组成,NdYAG棒直径为6 mm,Nd掺杂质量分数1%.在两个封装方式和结构一致的激光泵浦模块之间采用光学像传递和插入90°石英旋转片进行退偏补偿.在重复频率400 Hz,谐振腔输出单脉冲能量6 mJ时,双通输出400 mJ,激光器光-光转换效率为12.3%,光束质量4.6,脉宽15 ns.     

梯度折射率棒透镜的色差模型

本文提出一个梯度折射率棒透镜(GRIN－RodLens)的色差模型,并运用本模型合理地解释了在色差测量过程发现的各类色差现象.     

声学消息

随着激光技术的不断发展,对优质YAG激光晶体棒的需求量日益增加,但是,由于优质YAG晶坯获得不易,加之YAG晶体棒现行成形工艺存在一些不足,例如,取棒位置精度不准,影响取棒质量;晶坯出棒率低;加工生产率低等,不仅使优质晶体棒价格大大增加(一根直径5mm、长100mm以上的优质晶体棒,价格高达数千元,甚至近万元),而且还不能及时满足日益增长的需要,因此,从加工工艺角度,改革晶体棒的成形工艺是一项重要而迫切的任务.为此,电子部十