264～280 nm波段萘的共振增强多光子电离研究

在我们自己研制的具有恒温加热进样系统的激光质谱仪上实验获得了气相萘分子的共振增强多光子电离/飞行时间质谱(REMPI-TOFMS),以及萘母体离子C10H+8和一些主要碎片离子C8H+6、C6H+6、C5H+3、C4H+3、C3H+3在264～280 nm的分质量光谱.结合在266 nm激发波长下实验得到的这些离子的光强指数及不同激光能量下的分支比,对母体离子及主要碎片离子的生成机理进行了探讨:在该波段范围内,萘母体分子首先吸收一个光子从基态跃迁至激发态,激发态分子再吸收一个光子而电离产生母体离子C10H+8;碎片离子C8H+6、C6H+6、C5H+3、C4H+3、C3H+3则是由母体离子进一步吸收光子解离形成的,并给出了可能的解离通道.     

Lu2Si2O7：Ce晶体的闪烁性能

用提拉法生长了Lu2Si2O7：Ce晶体，对该晶体的闪烁性能进行了研究。透射光谱表明，Lu2Si2O7：Ce晶体的吸收边比Lu2SiO5：Ce晶体向短波方向移动了25nm，使透光范围进一步拓宽。X射线发射光谱和UV激发发射光谱均具有典型的双峰特征，主峰在378nm。UV激发发射谱具有温度效应，即375K以上时，发光效率迅速降低；425K以上时，发光主峰位明显红移。衰减曲线符合单指数式衰减规律，常温下经UV激发后的衰减时间约为34ns。从曲线形态看，375K以下的衰减谱与室温下的几乎完全相同，拟合的结果在32．8～34ns之间；衰减时间的温度效应从375K开始显现，即随温度的升高，衰减时间有加速变短的趋势，到500K时缩短为6．72ns。热释光谱在488，553K处有两个热释光峰，但室温附近几乎观察不到热释光峰。     

原子力显微镜在分子细胞生物学研究中的应用

 1986年秉霖(G.Binning)等在扫描隧道显微镜的基础上发明了原子力显微镜(Atomicforcemicro-scope,AFM)。这种显微镜的放大倍数远远超过以往的任何显微镜,可以直接观察物质的分子和原子组成,这为微观世界的探索提供了理想的工具。AFM不仅可以以高分辨率表征样品表面形貌,分析研究与作用力相对应的各种表面性质,并可对样品的分子或原子进行纳米级力加工,也能对活的生命样品进行实时动态观测。这些特性使AFM在生命科学特别是在分子细胞生物学的研究中占据着独特的地位。一、AFM对细胞表面结构的研究AFM的样品制备简单,只需作一个渗涂片并在空气中干燥,且不需特殊的染色和固定;它的     

CdSe和ZnO量子点的拉曼光谱研究

本文介绍了用拉曼光谱研究CdSe和ZnO两种Ⅱ Ⅳ族量子点材料的结果,对拉曼峰进行了指认。观察到的光学声子峰位的移动被认为是由量子限制效应引起。     

Singlet-Triplet Transition in Quantum Dots Confined by Triangular and Bowl-Like Potentials： the Effect of Electric Fields

We theoretically investigate the energy spectra of two-electron two-dimensional （2e 2D） quantum dots （QDs） confined by triangular potentials and bowl-like potentials in a magnetic field by exact diagonalization in the framework of effective mass theory. An in-plane electric field is found to contribute to the singlet-triplet transition of the ground state of the 2e 2D QDs confined by triangular or bowl-like potentials in a perpendicular magnetic field. The stronger the in-plane electric field, the smaller the magnetic field for the total spin of the ground states in the dot systems to change from S = 0 to S = 1. However, the influence of an in-plane electric field on the singlettriplet transition of the ground state of two electrons in a triangular QD modulated by a perpendicular magnetic field is quite small because the triangular potential just deviates from the harmonic potential well slightly. We find that the strength of the perpendicular magnetic field needed for the spin singlet-triplet transition of the ground state of the QD confined by a bowl-like potential is reduced drastically by applying an in-plane electric field.     

基于射频模块MAX2740设计的高动态GPS接收机前端

基于MAX2740射频接收前端提供了从天线到数字化输入之间完备的GPS接收方案，信号通道包括了低噪声放大器（LNA）、两级下变频器、可变增益／固定增益放大器、压控振荡器（VCO）及频率合成器等。     

高纯度烟草过氧化物酶(TOPⅠ)光谱特性研究

采用交换吸附脱色及柱层析新技术,成功地从烟叶中分离和纯化了一种烟草过氧化物酶同工酶(TOPⅠ),并对其进行了一系列光谱特性研究.基质辅助激光解吸电离飞行时间质谱(MALDI-TOF-MS)测得TOPⅠ分子量为21 888.5,等电点pI为3.5;氨基酸组成分析表明TOPⅠ为一含血红素的酸性蛋白酶.光谱学分析揭示,在402 nm处有一典型的Soret带,在498和636 nm处有特征吸收峰(α,β带),酸度和变性剂对TOPI在紫外可见区的特征吸收峰均产生一定的影响,TOP Ⅰ的荧光光谱测定结果说明TOPⅠ分子中含有Trp残基和Tyr残基以及其自身的独特的光谱学特性.     

氢原子光谱实验研究

氢原子的结构简单，其光谱具有明显的规律，各种原子光谱线规律性的研究首先是在氢原子上得到突破。通过测量氢光谱可见谱线的波长，能较准确测定氢的里德伯常数，可使学生对近代物理测量有初步了解。     

A Quasi-Symmetric Coupled Quantum Well and Its Electric-Optical Properties

We propose a novel coupled quantum well structure, i.e. a quasi-symmetric coupled quantum well (QSCQW). Based on the demands of optical switching devices for quantum well materials, the QSCQW configuration is further optimized. Consequently, in the case of low applied electric field 25kV/cm and low absorption loss 100cm^-1, a large field-induced refractive index change (for TE mode, n = 0.0106; for TM mode, n = 0.0115) is obtained in the QSCQW structure at the operation wavelength 1550hm. The value is in one or two order of magnitude larger than that in a rectangular quantum well and about 50% larger than that of five-step asymmetric coupled quantum well structure under the same working conditions. The refractive index change obtained with the optimized QSCQW under so low absorption loss and applied electric field is very attractive for semiconductor optical switching devices. This manifests that the QSCQW structure has a great potential for applications in ultra-fast and low-voltage optical switches and in travelling wave modulators.