Structural and luminescent characteristics of non-stoichiometric ZnO films by various sputtering and annealing temperatures

ZnO thin films were prepared by reactive RF magnetron sputtering at various deposition temperatures. They were annealed in oxygen ambient at various annealing temperatures. The microstructures and photoluminescence characteristics of ZnO films were investigated. The grain size of the ZnO thin film that was deposited at room temperature (RT) after annealing exceeded that of the film that was deposited at . Excess Zn atoms were considered to be present in the ZnO film that was deposited at RT, so the film was non-stoichiometric ZnO. No visible emission of either of the ZnO films deposited at the two temperatures was observed before annealing. Following annealing at high temperature, the green emission from the ZnO film that was deposited at RT was stronger than that of the film that was deposited at . The relationship between the non-stoichiometry of the thin film and the visible emission was discussed. The luminescent centers that correspond to green emission are defects; the concentration of defects was higher in the ZnO thin film that was deposited at RT than in the film that was deposited at .     

Spin accumulation in coupled quantum dots with ferromagnetic and superconducting electrodes

We theoretically investigate the spin accumulation in two parallel coupled quantum dots (QDs) with ferromagnetic and superconducting electrodes. Due to the ferromagnetic lead, the spin accumulation appears on the resonance of Andreev reflection. The spin accumulation in each of the two QDs can be controlled by the gate voltage. The sign of the spin accumulation is also controllable by tuning the bias. Furthermore, tuning the magnetic flux can exchange the amplitude of the spin accumulation in the two QDs. The Aharonov-Bohm oscillation effects also provides a way to control the spin accumulation of each QD.     

一种具有自适应非均匀校正功能的非制冷焦平面探测器组件

基于场景的非均匀校正算法(scene based nonuniformity correction,SBNUC)是非均匀校正技术今后的重点发展方向,介绍了近年来基于恒定统计约束的SBNUC、神经网络的SBNUC和运动估计的SBNUC算法的研究进展。研究了SBNUC算法在实际焦平面探测器组件上的实现方法,该方法仅依赖拍摄序列的信息对焦平面探测器的增益和偏置参数进行组间更新或帧间更新,可有效补偿温漂。研制了一种具有自适应非均匀校正功能的非制冷焦平面探测器组件,红外视频经该组件处理后,图像质量有所提高。该组件可明显提高热成像系统的成像性能,并能动态地保证热成像系统随场景变化的稳定性。     

激光模场传递矩阵分析方法的精度控制

讨论激光模场的传递矩阵分析法,并对计算精度进行控制.结果表明,传递矩阵分析方法与传统的积分数值迭代法计算结果一致,只要合理控制计算精度,可以解决积分数值迭代法难于收敛的问题,满足激光谐振腔模场分析的实际要求.     

低对比度小目标检测

对强杂波背景下的远距离目标探测,提出基于序列图像的局部自适应背景预测,获得图像背景的最佳估计。对残差图像采用能量累积及中值滤波消除背景杂波。为提高信噪比,采用带缓冲窗口的双窗滤波法使目标和背景的差别更加显著,有利于低对比度下的目标分割。最后采用改进的高阶相关方法,在不影响检测性能的情况下加快了真实目标识别的运算收敛速度,并最终实现了算法工程化,在图像局部信噪比大于0.3时,采用三阶相关时检测概率达到98%。     

X-射线荧光光谱法测定溶样后熔融制样金属硅中铁、铝、钙、钛、磷、铜

本文提出了溶解、蒸干然后用熔剂熔融残渣的样品制备方法,解决了金属硅不易直接熔融制样的难题,可以同时测定金属硅中多种杂质元素,消除了基体效应的影响,克服了标准样品对测定的限制,测定范围广,准确度高,通过安排正交试验确定了样品制备条件。     

化学工程中分形问题的正交配置法

将欧氏空间中的正交配置法扩展到分数维的情况,并将它应用于化学工程中具有分形结构的反应扩散问题的计算.并将计算结果与理论解的相应结果作了对比.     

特解边界元法数值解三维Pennes方程及其应用

应用特解边界元法对非稳态的三维Pennes方程求解,将解分为一满足泊松方程的通解与一特解之和,通解按照边界元法求解,特解用分离变量法给出,与位置有关的部分采用截断多项式.逐时间段计算边界元的温度及热流值,然后计算域内点的值.并将该方法用于热疗温度场的数值实例计算.     

Site Preference Model for Hyperfine Impurities in Compounds

A thermodynamic model for site preferences of solute atoms in ordered binary phases is applied in this paper for substitutional and interstitial sites of the Cu₃Au, or L1₂, structure. Site preferences are found to depend on formation energies of combinations of elementary point defects and on energies for transfer of solutes among different sites. The composition dependence in compounds having a wide phase field is examined in detail. A phenomenology of site preference behavior is outlined for regular lattice sites as well as for non-lattice sites such as grain boundaries. This revised version was published online in September 2006 with corrections to the Cover Date.     

Changes Brought about by a Lens in an Obliquely Incident Laser Beam

In the paraxial optics approximation, we have studied the transformation of a simple Gaussian beam of light obliquely incident on an isotropic lens for the case where the axis of the beam and the principal optical axis of the lens are crossed straight lines. The data obtained are compared with the corresponding results for the case where the axes of the beam and lens are coplanar.