光辐照对单根In掺杂ZnO纳米线电学性质的影响

通过化学气相沉积方法成功制备了高质量的In掺杂ZnO纳米线.选用325 nm的He-Cd激光器做为光源,进一步探究了单根In掺杂ZnO纳米线的光响应特性.结果表明:紫外光辐照可使金属电极与纳米线之间的有效肖特基接触势垒下降,使接触类型由肖特基接触转变到欧姆接触;撤去紫外光后,电极与纳米线之间的接触可以恢复到未光照时的肖特基接触.讨论了肖特基接触与欧姆接触之间转变的物理机制.     

Wavefront correction of Ti:sapphire terawatt laser with varying precision of phase conjugation between deformable mirror and wavefront sensor

The phase conjugation between the deformable mirror and the wavefront sensor in the aberration correction of a terawatt Ti:sapphire laser is studied experimentally and theoretically in this paper. At varying values of phase-conjugation precision, we focus the corresponding beams into spots of the same size of 5.1 μm×5.3 μm with a f/4 parabola in the 32 TW/36 fs Ti:sapphire laser system. The results show that the precision of conjugation can induce an intensity modulation but does not significantly affect the wavefront correction.     

电子的发现与化学键电子理论的发展

1892年,荷兰物理学家洛伦兹通过创建电子论,为原子内部电子的发现提供了理论基础。1897年,英国物理学家汤姆逊从阴极射线中发现了自由电子,打破了原子不可分的传统观念,由此引发了卢瑟福、玻尔等人对原子内部结构的探索。同时,化学家们将物理学中的电子引入化学,开始用原子结构中的电子来解释化学行为,提出了化学键的电子理论,推动了化学键理论的发展。     

室温下快速合成均质大颗粒有机-无机杂化钙钛矿薄膜

在室温下,采用超声辅助液相法快速合成了有机-无机杂化钙钛矿薄膜.碘化铅和甲基碘化氨的摩尔比为1∶1,通过超声振荡法溶于γ-丁内酯(GBL)溶液,得到黄色透明液体.采用荧光分光光度计对溶液的光发射谱进行表征,发现在495 nm和826 nm出现特征峰;采用滴涂法以及溶剂蒸发来制备有机-无机杂化钙钛矿薄膜,通过XRD和SEM对薄膜结构和形貌进行分析.结果表明,获得的钙钛矿薄膜是四方晶系,薄膜的晶粒呈现不规则的六边形且尺寸达到微米量级.     

基于局部相关性的遥感图像全色锐化算法

为了增强多光谱图像的空间分辨率同时避免出现严重的光谱扭曲,对插值放大后的多光谱图像和原始全色图像分别作相同层数的非下采样轮廓波变换分解.在相应低频子带中,分别选取以待融合像素点为中心,大小为5×5的滑动窗口,计算待融合像素点的局部相关系数与四阶相关系数.如果局部相关系数大于四阶相关系数,说明该位置上的地物存在相似的光谱特征,因此用全色图像的高频系数替代多光谱图像的高频系数;反之,保持多光谱图像的高频系数不变.最后将多光谱图像的低频系数和替换后的高频系数进行非下采样轮廓波逆变换得到融合图像.采用Landsat 7遥感图像,对比给出了本文与现有同类最新文献融合结果及其主客观评价指标.实验结果表明,本文算法在提高空间分辨率与保持光谱信息两个方面都具有较好的效果.     

基于稀疏表示的可见光遥感图像飞机检测算法

为解决当前遥感图像飞机检测方法在复杂背景下准确率低,实现旋转不变困难的问题,结合图像稀疏表示原理,提出一种基于稀疏表示的飞机检测算法.该算法首先利用飞机是刚性目标且具有明显几何外观的特点,构建飞机几何原子库;然后建立飞机轮廓几何逼近的最优化方程,在稀疏表示原理框架下,得到飞机轮廓最优的几何部件组合;最后,以星型结构的部件模型为框架,生成待检测图像的目标显著图并根据显著图定位出飞机.实验结果表明,稀疏表示方法能自适应选取飞机部件,部件数目较少且不易受光照、颜色和复杂背景的影响.与现有算法相比,本文算法准确率达90%以上,检测速度有较大的提高.     

Can contributions to B_s→l＋l-γ from the magnetic-penguin operator with real photons in the standard model be neglected？

Using the Bs meson wave function extracted from non-leptonic Bs decays, we reevaluate the rare decays Bs→l＋l- γ,（l=e,μ） in the Standard Model, including two kinds of contributions from the magnetic-penguin operator with virtual and real photons. We find that contributions to the exclusive decays from the magnetic-penguin operator b→sγ with real photons, which were regarded as negligible in the previous literature, are large and the branching ratios Bs→l＋l-γ are enhanced by a factor of almost 2. With the predicted branching ratios of the order of 10-8, it is expected that these radiative dileptonic decays will be detected in LHC-b and B factories in the near future.     

Can contributions to B_s→l~+l~-γ from the magnetic-penguin operator with real photons in the standard model be neglected?

Using the Bs meson wave function extracted from non-leptonic Bs decays, we reevaluate the rare decays Bs→l+l- γ,(l=e,μ) in the Standard Model, including two kinds of contributions from the magnetic-penguin operator with virtual and real photons. We find that contributions to the exclusive decays from the magnetic-penguin operator b→sγ with real photons, which were regarded as negligible in the previous literature, are large and the branching ratios Bs→l+l-γ are enhanced by a factor of almost 2. With the predicted branching ratios of the order of 10-8, it is expected that these radiative dileptonic decays will be detected in LHC-b and B factories in the near future.     

Electron Dynamics of Atoms in Parallel Electric and Magnetic Fields

Through an analysis of the nearest neighbor level fields, we investigate the evolution of the electron spacing statistics for atoms in parallel electric and magnetic dynamics as electric field strength increases. In the ＇inter-l mixing＇ predominant region, the electron shows complex dynamics while in the ＇inter-n mixing＇ predominant region, its dynamics behaves in a relatively stable way and the characteristic quantity ξ shows a slight oscillation. Comparing the dynamics for hydrogen and barium, we find that the core effect makes the main contribution to the chaotic behavior in non-hydrogen atoms.