第一讲 光电子器件在光纤通信中的应用

光纤通信技术发展的阶段性飞跃总是伴随新型光电材料和功能器件的突破.文章介绍了光纤通信系统中应用到的各种光电子器件,从光纤通信的3个环节：光发送、光接受、光放大为出发点,着重阐述了半导体激光器、光调制器、光检测器、光放大器等关键器件的基本原理、工作特性以及发展现状和趋势,并在回顾传统集成光电子器件发展的同时,展望了以新一代微纳结构光电子器件为基础的光子集成技术的发展趋势.     

Origin 8.5在亥姆赫兹线圈磁场测量实验数据处理中的应用

与传统的人工处理实验数据相比,Origin8.5软件处理实验数据具有方便快捷、直观、精度高等特点。文中通过使用Origin8.5软件处理亥姆赫兹线圈测磁场实验的数据,详细介绍了二维绘图、三维绘图以及非线性曲线拟合的过程,结果表明使用Origin8.5软件处理实验数据能有效的减少人工处理带来的误差。     

Fuzzy Impulsive Control of Permanent Magnet Synchronous Motors

The permanent magnet synchronous motors （PMSMs） may experience chaotic behaviours with systemic parameters falling into a certain area or under certain working conditions, which threaten the secure and stable operation of motor-driven. Hence, it is important to study the methods of controlling or suppressing chaos in PMSMs. In this work, the Takagi-Sugeno （T-S） fuzzy impulsive control model for PMSMs is established via the T-S modelling methodology and impulsive technology. Based on the new model, the control conditions of asymptotieal stability and exponential stability for PMSMs have been derived by the Lyapunov method. Finaily, an illustrated example is also given to show the effectiveness of the obtained results.     

Design of Broadband Single Fundamental Mode Hollow Core Bragg Fibre

The condition of the single fundamental mode （HE11） transmission in hollow core Bragg fibres is investigated theoretically by the transfer matrix method. The influences of core size and cladding parameters on the single HE11 mode bandwidth are analysed, showing that the maximal bandwidth is more sensitive to the core size than the cladding. The numerical results show that sufficiently broad bandwidth of single HE11 mode transmission can be achieved by proper fibre design. A simple and fast method based on improved hollow metal waveguide model is proposed to optimize fibre structure parameters for the maximal single HE11 mode bandwidth.     

核计算技术在核测井中的应用

本文介绍了核计算技术在核测井中的应用概况及其具体应用实例。     

AlB+n(n=2～10)团簇结构和红外振动光谱研究

用密度泛函理论的B3LYP方法在6-311G(d)水平上对AlB+n(n=2～10)团簇几何结构、稳定性、电子结构和成键特性进行了系统理论研究,得到了AlB+n(n=2～10)团簇的最稳定结构.结果表明,硼原子间容易聚集,铝原子处于整个硼原子集团的外围.与相应中性AlBn团簇相比,Al-B键作用变弱,使正价团簇(n=6...     

Analysis of Ar line spectra from indirectly-driven implosion experiments on SGII facility

This paper reports on the indirectly-driven implosion experiments on SGII laser facility in which Ar emission spectrum from Ar-doped D-filled plastic capsule is recorded with the crystal spectrometer. Spectral features of Ar Heβ line and its associated satellites are analysed to extract the electron temperature and density of the implosion core. Non local thermal equilibrium (NLTE) collisional-radiative atomic kinetics and Strark broadening line shape are included in the present calculation. By comparing the calculated spectrum with the measured one, the core electron temperature and density are inferred to be 700 eV and 2.5×10²³ cm^-3 respectively. With these inferred values of electron temperature and density, neutron yield can be estimated to agree with the measured value in magnitude despite of the very simple model used for the estimation.     

O2流量对磁控溅射N掺杂TiO2薄膜成分及晶体结构的影响

利用直流脉冲磁控溅射方法在室温下通过改变O₂流量制备具有不同晶体结构的N掺杂TiO₂薄膜,利用台阶仪、X射线光电子能谱仪、X射线衍射仪、紫外-可见分光光度计等设备对薄膜沉积速率、化学成分、晶体结构、禁带宽度等进行分析.结果表明:所制备的薄膜元素配比约为TiO_1.68±0.06N_0.11±0.01,N为替位掺杂,所有样品退火前后均未形成Ti—N相结构,N掺杂TiO₂薄膜的沉积速率、晶体结构等主要依赖于O₂流量.在O₂流量为2 sccm时,N掺杂TiO₂薄膜沉积速率相对较高,薄膜为非晶态结构,但薄膜内含有锐钛矿(anatase)和金红石(rutile)相晶核,退火后薄膜呈anatase和rutile相混合结构,禁带宽度仅为2.86 eV.随着O₂流量的增加,薄膜沉积速率单调下降,退火后样品禁带宽度逐渐增加.当O₂流量为12 sccm时,薄膜为anatase相择优生长,退火后呈anatase相结构,禁带宽度为3.2 eV.综合本实验的分析结果,要在室温条件下制备晶态N掺杂TiO₂薄膜,需在高O₂流量(＞10 sccn)条件下制备. 关键词： 2薄膜')" href="#">N掺杂TiO₂薄膜 磁控溅射 化学配比 晶体结构     

循环伏安法研究Ba2YCu3O7—y超导体

本文利用电化学循环伏安法(CV 法),以饱和 Ba(OH)_2水溶液为电解液,对单相Ba_2YCu_3O_(7-y)正交和四方结构超导体进行了研究.结果发现:在典型的正交相中确实存在Cu~(3+)→Cu~(2+)的还原峰,而四方相则无此峰出现.从而首次直接检测到 Ba_2YCu_3O_(7-y)烧结体中 Cu~(3+)离子.     

A New Method for Calculating the Thermoelectric Efficiency

We present an approximate method for calculating the thermoelectric efficiency. The method has a high precision and is applicable to almost all of the thermoelectric devices. The expression for the thermoelectric efficiency we obtained does not involve the position variable, so the calculations are simplified greatly.