KTiOPO4晶体纵横模劈裂的喇曼谱

在室温下测量了ＫＴｉＯＰＯ₄单晶的偏振喇曼散射谱，应用９０°散射及背散射得到了各模的峰位值，其中Ｂ₁（ＬＯ）模、Ｂ₂（ＬＯ）模的喇曼谱测量尚未见报道过。根据ＬＯ－ＴＯ劈裂的实验结果，计算出该晶体极化模的有效电荷、振子强度及沿对称轴方向的静态介电常数。 关键词：     

脉冲红外激光诱发SiH4+CH4解离动力学研究

采用光学发射谱（ＯＥＳ）技术对脉冲ＴＥＡ ＣＯ₂激光诱发ＳｉＨ₄＋ＣＨ₄系统击穿产生的等离子体辐射进行了时间分辨的光谱测量。结果表明等离子体内分子的各碎片发光均在气体击穿时刻开始出现，但具有不同的时间特性，由此探讨了气体分子的分解过程。分析结果支持激光诱发ＳｉＨ₄＋ＣＨ₄等离子体内的主要离解通道为产生Ｓｉ，Ｃ原子通道的分解动力学机制的解释。据此观点讨论了气体分解碎片间的反应过程。实验与理论符合较好。 关键词：     

Cs原子里德伯态Stark能级场电离阈值与｜ml｜关系的测定

报道Ｃｓ原子里德伯态Ｓｔａｒｋ能级场电离阈值与｜ｍ_l｜依赖关系的实验研究结果，从实验上同时测得Ｃｓ原子｜ｍ_l｜＝０，１，２三种态的电离阈值表达式。 关键词：     

三元合金Cu76Ni15Sn9的离子溅射研究

在２７ｋｅＶ Ａｒ⁺离子轰击时,用收集膜技术结合俄歇谱仪（ＡＥＳ）,研究了三元合金Cu₇₆Ni₁₅Sn₉系统的择优溅射行为。同时使用扫描电子显微镜（ＳＥＭ）与电子探针微分析（ＥＰＭＡ）．观察了靶点表面形貌变化并测定了形貌特征微区的合金组份原子的相对百分浓度。结果表明,Ｃｕ原子较Ｎｉ原子、Ｎｉ原子较Ｓｎ原子,在所测定范围（０─６０°）内择优发射。最后讨论了靶点表面形貌特征和“元素局域富集”现象对择优溅射过程的影响。 关键词：     

线阵扫描超声相关合成成像方法与实验

本文讨论了改进的医用B超线阵扫描探头在工业无损检测中的应用．在合成孔径聚焦技术（SAFT）基础上提出了改进方法，在探元响应带宽较窄的情况下可获得较高信噪比的成像结果．文中介绍了成像系统，实验方法，并给出了一些实验结果．     

p-GaN层厚度对GaN基p-i-n结构紫外探测器性能的影响

研究了p-GaN层厚度对GaN基pin结构紫外探测器性能的影响.模拟计算表明：较厚的p-GaN层会减小器件的量子效率,然而同时也会减小器件的暗电流,较薄的p-GaN层会增加器件的量子效率,但是同时也增加了器件的暗电流.进一步的分析表明,金属和p-GaN之间的结电场是出现这种现象的根本原因.在实际的器件设计中,应该根据实际需要选择p型层的厚度. 关键词： GaN 紫外探测器 量子效率 暗电流     

Convergent-beam electron diffraction of CaZr4O9, a complex zirconia alloy phase

The point-group and space-group symmetry of the controversial fluorite-based stoichiometric superlath phase of ø₁ (CaZr₄O₉: Z=16), considered to be a coherently-intergrown subphase of lime-stabilized zirconia, is examined. Using convergent-beam and selected-area electron diffraction, it is determined that the space group of ø₁ is C2/c, in apparent agreement with earlier studies utilizing other diffraction techniques.     

Creation of variable concentrations of defects on TiO2(110) using low-density electron beams

Low density (˜μA/cm²) 0.48 and 1.0 keV electron beams have been used to create surface defects on a TiO₂(110) surface. These electron-beam induced defects were examined primarily by X-ray photoelectron spectroscopy (XPS) with supporting ultraviolet photoemission spectroscopy (UPS). Glancing and normal emission XPS spectra of nearly defect-free surfaces revealed that Ti atoms on the surface were similar to the bulk Ti, while some surface oxygen atoms were different from the bulk oxygen. XPS of Ti 2p_3/2 was used to quantify the defect concentration and to examine the defect electronic structure. Based on our calculation of defect concentrations and the comparison of our results with results and models from the literature, we conclude that oxygen vacancies induced by electron beams in the current study are mostly from the bridging oxygen sites, in agreement with the previous work. A range of defect concentrations with similar electronic structure, mainly composed of Ti³⁺, have been induced by low-density electron beams. Beam energy and exposure were the experimental variables. The rates of defect formation at low beam exposure were beam-energy dependent, with a faster growth rate at 0.48 keV than at 1.0 keV. These defects were similar to those by thermal annealing in vacuum, but a higher concentration of defects could be obtained with longer beam exposure. However, the e-beam induced defects were different from those produced by Ar⁺ ion bombardment since both this and previous studies have found defects produced by Ar⁺ ion bombardment to be complex, with a variety of different local environments where oxygen and titanium surface atoms coexist.     

Ti:sapphire second-harmonic-pumped visible range femtosecond optical parametric oscillator

A β-barium borate (BBO) femtosecond optical parametric oscillator (OPO) pumped by the second-harmonic of a modelocked 82 MHz Ti:sapphire laser is described. With intracavity dispersion compensation, pulse durations down to 30 fs are obtained with a total average power up to 100 mW. The current wavelength range, with a 400 nm pump, is from 566 nm to 676 nm. Unusual tuning characteristics, including bichromatic emission, are presented in detail and explained theoretically.     

Thick grids with circular apertures: A comparison of theoretical and experimental performance

In this paper a comparison between a rigorous electromagnetic model for transmission through a hexagonal array of circular waveguides in a series of thick, metallic screens and experimental measurements in the far infrared is made. It is found that there is excellent agreement between theory and experiment when the frequency is below that where any diffracted orders propagate. The agreement is still very good above this frequency. Below a frequency approximately equal to the cut-off frequency of the circular waveguides little power is transmitted. As the thickness of the screen is increased, this decrease in transmission becomes more abrupt. Also, for thick screens, resonances appear in the transmission spectrum which are analogous to those which appear in the spectra of two grids separated by a distance comparable to the wavelength of the radiation being used.