入射角和杂质吸收对一维光子晶体反射镜的影响

利用复折射率的方法和膜系设计软件TFcalc分别研究了入射角和杂质吸收对一维光子晶体反射镜反射谱和透射谱的影响.结果表明:随着入射角的增大,一维光子晶体反射镜的禁带中心位置蓝移,禁带宽度减小.入射角小于60°时,带隙势阱深度几乎不变,大于60°后带隙势阱深度变化较大.当入射角无限接近90°时,P偏振光的带隙几乎消失,S偏振光的带隙几乎保留.杂质吸收对于一维光子晶体的反射谱和透射谱显著影响时的临界消光系数值分别是0.001和0.0003.高折射率介质层的杂质吸收对光谱的影响较小.     

The solution to the BCS gap equation and the second-order phase transition in superconductivity

The existence and the uniqueness of the solution to the BCS gap equation of superconductivity are established in previous papers, but the temperature dependence of the solution is not discussed. In this paper, in order to show how the solution varies with the temperature, we first give another proof of the existence and the uniqueness of the solution and point out that the unique solution belongs to a certain set. Here this set depends on the temperature T. We define another certain subset of a Banach space consisting of continuous functions of both T and x. Here, x stands for the kinetic energy of an electron minus the chemical potential. Let the solution be approximated by an element of the subset of the Banach space above. Second, we show, under this approximation, that the transition to a superconducting state is a second-order phase transition.     

A note on the integrality gap of an ILP formulation for the periodic maintenance problem

We address the integrality gap of the integer linear program introduced by Grigoriev et al. (2006) [3] for the periodic maintenance problem. We prove that the integrality gap of this program is bounded by a constant.     

Reflection and transmission of plane acoustic waves in an infinite annular duct with a finite gap on the inner wall

The diffraction of acoustic waves by an infinitely long annular duct having a finite gap on the inner wall is investigated rigorously. The related boundary‐value problem is formulated into a modified Wiener–Hopf equation, which is then reduced to a pair of simultaneous Fredholm integral equations of the second kind. At the end of the analysis, numerical results illustrating the effects of the width of the coaxial cylindrical waveguide and the gap length on the diffraction phenomenon are presented. Copyright © 2010 John Wiley & Sons, Ltd.     

二氧化硅蛋白石光子晶体中粒子重构对光学性质的影响

使用自组装法制备了蛋白石结构二氧化硅纳米球三维光子晶体,并对样品在150,300,450℃温度下进行了热处理.随热处理温度的升高,光子晶体禁带中心波长出现22.5 nm的蓝移,且禁带宽度变窄.对于在450℃热处理的样品,其测量的禁带中心波长为572.5 nm,与理论计算结果有较大差异.引起样品光学特性变化的原因是热处理...     

超薄氢化非晶锗膜的结构与光电性质

通过PECVD制备出了不同厚度的a-Ge∶H膜,采用Raman光谱对样品进行了结构表征,由椭圆偏振光谱仪得到样品的厚度和光学常数,并计算了样品的光学带隙。由变温电导率分析了薄膜的电学输运性质,结果表明,载流子的传输机制为扩展态电导。进而利用变温PL谱研究了薄膜的发光性能,发现其发光峰在1.63 μm处;随着膜厚的减小,峰位和峰形都有改变,且强度明显提高。进一步分析发现,随着膜厚的减小非辐射复合跃迁的激活能增大,从而导致辐射复合过程增强。     

拼接光栅缝隙对激光脉冲光强分布的影响

以拼接光栅作为色散元件的激光脉冲压缩器中,要求脉冲压缩光栅表面光强分布均匀、能量输出效率高。利用菲涅耳-基尔霍夫衍射原理对脉冲压缩光栅表面光强和远场光强分布进行了研究。计算了拼接光栅缝隙宽度对光栅表面光强变化量和远场光强极大值的影响。在利特罗角附近入射时发现激光脉冲光强分布与拼接光栅缝隙宽度相关,得出了光栅拼接缝隙宽度应控制在0.5 mm以内。适当提高缝隙衍射效率能够改善光强分布均匀性和提高光能量输出,提出了对拼接缝隙采用两次重复曝光以提高其衍射效率的方法。     

新型铁基超导体角分辨光电子能谱研究

最近发现的新型122结构的铁基超导体掀起了铁基高温超导研究的又一轮热潮.文章利用角分辨光电子能谱实验手段,研究了这类新型铁基材料的电子结构、费米面拓扑和超导能隙.实验结果表明,其在布里渊区中心的能带结构及费米面与其他铁基超导体存在明显差异,并导致嵌套在粒子-空穴通道的费米面消失.另外,在布里渊区边缘的电子型费米面发现了较强的并且有各向同性的超导能隙.这些结果对可能的超导配对机制提出了严格的限制.     

Low-frequency band gaps in one-dimensional thin phononic crystal plate with periodic stubbed surface

Using supercell plane wave expansion method, the Lamb wave band structure of one-dimensional thin plate with periodic stubs is investigated. The numerical results show that flat bands will appear and band gap can exist in a low-frequency domain. The position of the flat bands and width of the low-frequency Lamb wave band gap can be tuned by the stub height, plate thickness and filling fraction. The band gap is obtained by opening the folding points of the same plate modes not the crossing point of different plate mode when the stub height is small.     

Structural and optical properties of low temperature synthesized Nanostructured BiFeO3 thin films

Nanostructured bismuth ferrite (BiFeO₃) thin films were deposited on glass substrate by the sol-gel process. The as-fired film at 250 °C was found to be amorphous crystallizing to pure rhombohedral phase after annealing at 450 °C for 2 h in air. The XRD pattern shows that the sample is polycrystalline in nature. The average grain size of the film calculated from the XRD data was found to be 16 nm. The as-fired film show high transmittance that decreases after crystallization. The absorption edge of the films was found to be sharper and shifting towards the lower energy as the annealing temperature increases. The optical energy band gaps of the amorphous and crystalline films were found to be 2.63 and 2.31 eV, respectively. The refractive indices of the amorphous and crystalline films were 2.05 and 2.26, respectively.