基于单法布里-珀罗标准具的双频率四边缘鉴频光电探测技术

提出了一种基于单固体法布里-珀罗(F-P)标准具和可调谐半导体激光器的高精度鉴频新技术双频率四边缘技术。导出了F-P标准具反射谱和透射谱函数表达式,分析了双频率四边缘技术的鉴频原理;根据鉴频原理,给出了鉴频系统结构及相应的探测信号分析处理方法;进一步分析了噪声引起的测量误差,导出了具体的误差公式;与传统的基于F-P标准具双边缘鉴频技术的探测性能做了对比分析。结果表明,该技术通过对F-P标准具的透射和反射信号同时探测,鉴频精度将提高2.82~3.03倍,而且由于采用的是单固体F-P标准具,光路简单且系统成本低。     

J—196光电经纬仪大孔径高分辨率光学系统研究

J—196光电经纬仪是一个近距离、快速的小目标测量系统，同步高速摄影机是一个重要的测量手段，它配置了大孔径、高分辨率的摄影光学系统，与国内外光电经纬仪相比，它的相对孔径居首位，即在焦距f′=750，1500mm，口径为D=200mm，相对孔径达D/F=1：3.75，1：7.5，而它的成像质量是优良的。经检测，摄影分辨率达到N=561p/mm，超过了国内先进水平。     

不同浓度的尾砂胶结充填体破坏过程 声发射特性试验研究*

制备了3种不同质量浓度的充填体试件,进行了单轴压缩声发射试验,分析了不同浓度的充填体力学特性,重点研究了试件破坏过程中的声发射振铃计数、声发射累计撞击数与声发射累计能量的比值(r值)、主频及其相对高频信号激增响应系数特征。研究表明：随着浓度的增加,充填体的峰值强度与弹性模量呈增大趋势,充填体中出现的声发射累计振铃计数越多;r值先升高再持续减小到一个较低值,随着外载荷的增加,进入缓慢升高阶段,峰值前均保持在该阶段。充填体破裂前兆信息在声发射信号主频分布中呈现主频段增多现象,表现为由加载初期的1~2个主频段,在临界主破裂时增多到3~5个主频段;且随着浓度的增加,声发射信号主频频段分布越宽,声发射相对高频信号(160~180 kHz)的激增响应系数呈递减趋势。以上特征可为不同浓度的尾砂胶结充填体稳定性监测、预测提供依据。     

硼掺杂富勒烯储氢-从物理吸附到化学吸附的转变

本文采用密度泛函理论(DFT)中的局域密度近似(LDA)方法对硼(B)掺杂富勒烯(C_(35)B)储氢问题在前人的基础上做了进一步研究,结果表明被C_(35)B吸附的氢分子很容易解离,经历从物理吸附到化学吸附的转变,并且发现解离产物C_(34)BHCH有分子内氢转移反应发生,这时B原子仍能与氢分子有很强的相互作用,最终导致B位置以及与B最邻近的三个C原子上都有氢原子吸附.并利用过渡态理论从热力学上分析了这种反应的发生趋势.     

面向情感语音转换的韵律转换方法

面向情感语音转换,该文提出了一种韵律转换方法。该方法包含基频转换和时长转换两个部分,前者选择离散余弦变换(DCT)参数化基频,根据基频的层次结构特点,将基频分解为短语层和音节层两个层次,使用基于混合高斯模型(GMM)的转换方法对两个层次分别进行转换;后者使用基于分类回归树(CART)的方法以声韵母为基本单位对时长进行转换。一个包含三种基本情感的语料库用作训练和测试,客观评测以及主观评测实验结果显示该方法可有效进行情感韵律转换,其中悲伤情感在主观实验中达到了接近100%的正确率。      

500—4250eV电子对CO2的散射全截面绝对测量

对中能电子与二氧化碳分子碰撞的散射全截面测量，给出５００－４２５０ｅＶ电子对ＣＯ２的绝对散射全截面。对测量结果作了曲线拟合，并与已有的实验和理论结果进行了比较     

Result of search for low velocity exotic particles

The L3＋C experiment, taking advantage of the L3 muon magnetic spectrometer, measured the spatial tracks of charged cosmic ray particles to obtain rigidity as well as velocity. One possible low velocity exotic particle is observed. The existing uncertainties are discussed, and the flux upper limit of the low velocity exotic particles from this observation is deduced based on the assumption of a null observation. The result is 6.2×10^-10 cm^-2·s^-1·sr^-1 at 90% confidence level in the velocity range from 0.04c to 0.5c.     

基于腔辅助相互作用的远距离信息传递

提出了一种基于腔辅助相互作用的远距离信息传递的方案.在该方案中,通过让一束相干光和一个囚禁在腔里面的原子进行相互作用,可以使相干光产生一个可控的相位偏移.用这种腔辅助相互作用完成了原子态和光场态之间信息的相互转移.最后我们演示了远距离信息传递方案,该方案在当前实验条件下是可行的,并且在理想条件下,成功的概率几乎为1.     

Self-organization effect in poly（3-hexylthiophene）： methanofullerenes solar cells

This paper studies the self-organization of the polymer in solar cells based on poly（3-hexylthiophene）： [6, 6]-phenyl C61-butyric acid methyl ester by controlling the growth rate of active layer. These blend films are characterized by UV-vis absorption spectroscopy, charge-transport dark J - V curve, x-ray diffraction pattern curve, and atomic force microscopy. The results indicate that slowing down the drying process of the wet films leads to an enhanced selforganization, which causes an increased hole transport. Increased incident light absorption, higher carrier mobility, and balanced carrier transport in the active layer explain the enhancement in the device performance, the power conversion efficiency of 3.43% and fill factor up to 64.6% are achieved under Air Mass 1.5, 100 mW/cm^2.     

Analytic solutions for degenerate Raman-coupled model

The Raman-coupled interaction between an atom and a single mode of a cavity field is studied. For the cases in which a light field is initially in a coherent state and in a thermal state separately, we have derived the analytic expressions for the time evolutions of atomic population difference W, modulus B of the Bloch vector, and entropy E. We find that the time evolutions of these quantities are periodic with a period of π. The maxima of W and B appear at the scaled interaction time points τ- = kπ（k = 0, 1, 2,...）. At these time points, E = 0, which shows that the atom and the field are not entangled. Between these time points, E ≠ 0, which means that the atom and the field are entangled. When the field is initially in a coherent state, near the maxima, the envelope of W is a Gaussian function with a variance of 1/（4n^-）（n^- is the mean number of photons）. Under the envelope, W oscillates at a frequency of n^-/π. When the field is initially in a thermal state, near the maxima, W is a Lorentz function with a width of 1/n^-.