负折射率材料对产生Casimir排斥力的影响

研究了负折射率材料对产生Casimir排斥效应的影响. 两材料板间的Casimir排斥力的发生取决于两板以及其间媒质的电磁特性,通过理论与数值结果的分析研究给出电磁特性所影响排斥力的产生趋势. 对于由Drude-Lorentz型色散关系描述等效介电常数和磁导率的负折射率材料,调节各特征频率参数可实现Casimir排斥效应. 关键词： Casimir排斥力 负折射率材料 Drude-Lorentz型色散关系     

二维情况下内部有质量费米子单圈图对Casimir力的贡献

采用Feynman的路径积分量子化方法,计算出两个平行的、理想的金属线之间,在绝对零度下量子电磁场在有质量费米子单圈图近似下的Casimir效应.     

非平行导线型边界下Maxwell-Chern-Simons场的Casimir效应

在路径积分量子化框架下，利用复变函数论中的保角变换与Plana求和公式，计算了（2＋1）维空间中两个非平行导线型边界下Maxwell-Chern-Simons场的Casimir效应.不引入任何截断参数，而得出有限的解析表达式. 关键词： Casimir效应 路径积分 保角变换 Plana求和公式     

用于超快、高效系统的半导体纳米结构光子器件

首先对未来系统光子器件的关键问题进行了综述。并且对半导体纳米结构,特别是基于量子点材料的超快开关器件取得的最新进展进行了讨论。其中包括基于量子点的半导体光放大器,其在超过40Gb/s的速率下展现出偏振不敏感特性;新型基于量子点的垂直腔结构的光开关,其展现出超快、节能、全光开关的特性。概括和讨论了未来基于纳米结构的光子器件的应用。     

基于半导体量子点的片上手性纳米光子器件

手性量子光学在量子信息技术研究领域中受到了广泛的关注,其主要研究光在微纳结构中自旋依赖的手性耦合及传输行为。利用手性光与物质的相互作用可以增强光子与量子发射器的耦合,赋予纳米光子器件新的功能和应用,从而推动手性量子光学在量子信息领域中的大规模应用。主要对基于半导体量子点的片上手性纳米光子器件进行了综述,重点讨论了半导体量子点的光学性质和手性光与物质相互作用的物理机制,在此基础上对近年来应用手性耦合原理实现的多功能手性光子器件进行了总结,并对手性量子光学的未来应用场景进行了展望。     

有限口径非周期亚波长衍射聚焦偏转器的严格矢量优化

有限口径非周期亚波长衍射光学器件的亚波长结构特性使得传统标量衍射理论失效,必须借助严格电磁理论进行器件的设计。提出一种循环平面波谱算法(IterativePlaneWaveSpectrumAlgorithm,IPWSA)作为器件优化算法,利用二维时域有限差分方法作为严格电磁计算模式,根据Farn方法对器件面型进行亚波长处理,设计出有限口径非周期具有亚波长结构的衍射聚焦偏转器件,偏转角为24.8°,该器件可与激光器集成构成微型集成光学系统,也可以用在红外量子阱系统中。详细分析了算法原理,设计实例验证了算法的优化效果。     

基于低次插值的红外焦平面器件非均匀性多点校正算法

提出了分段线性插值和三次样条插值两种基于低次插值的红外焦平面阵列非均匀性多点校正算法,该算法能有效地克服工程上常用的一点和二点校正算法的不足,具有校正精度高、动态范围大、在线计算量小、易于实时实现等优点,并且能有效克服IRFPA各探测单元响应特性的非线性对校正精度的影响.     

Repulsive Casimir Force in a Cavity Comprising a Dielectric with Output Coupling

The Casimir force between a perfectly conducting wall and a dielectric wall in a cavity comprising a transparent dielectric with output coupling is investigated. By using full quantum theory, we obtain the analysis expression of the force, which shows that the interaction of the two walls in this system is always repulsive. And the value of the Casimir force varies with the field amplitude reflectivity and the cavity size.     

Repulsive Casimir Force in a Cavity Comprising a Dielectric with Output Coupling

The Casimir force between a perfectly conducting wall and a dielectric wall in a cavity comprising a transparent dielectric with output coupling is investigated. By using full quantum theory, we obtain the analysis expression of the force, which shows that the interaction of the two walls in this system is always repulsive. And the value of the Casimir force varies with the field amplitude reflectivity and the cavity size.     

Maxwell-Chern-Simons Casimir Force Between Perfectly Conducting Parallel Lines

Using Feynman path integral method we calculate the Casimir force of Maxwell-Chern-Simons Abelian gauge field between perfectly conducting parallel lines.     

Maxwell-Chern-Simons Casimir Force Between Perfectly Conducting Parallel Lines

Using Feynman path integral method we calculate the Casimir force of Maxwell Chern Simons Abelian gauge field between perfectly conducting parallel lines.``     

Casimir Force on a Piston in Randall-Sundrum Models

The Casimir effect of a piston for massless scalar fields which satisfy Dirichlet boundary conditions in the context of five-dimensional Randall- Sundrum models is studied. In these scenarios we derive and calculate the expression for the Casimir force on the piston. We also discuss the Casimir force in the limit that one outer plate is moved to the remote place to show that the nature of the reduced force between the parallel plates left. In the Randall~undrum model involving two branes the two plates attract each other when they locate very closely, but the reduced Casimir force turns to be repulsive as the plates separation is not extremely tiny, which is against the experimental phenomena, meaning that the RSI model can not be acceptable. In the case of one brane model the shape of the reduced Casimir force is similar to that of the standard two-parallel-system in the four-dimensional fiat spacetimes while the sign of force remains negative.     

Casimir Force in a One-Dimensional Cavity with Quasimode

We calculate the Casimir force between a perfect reflective wall and a semitransparent wall in the laser cavity. Using the Fox-Li quasimode theory to describe the electromagnetic field in the laser cavity, the vacuum energy and the Casimir force are calculated. We compare our results to the force in the ideal situation and find it smaller in the dissipative cavity. We also find that the Casimir force decreases with the increase of the wall-wall distance and the decay rate of the quasimodes in the laser cavity.     

Casimir Force at a Finite Cut-Off

We calculate the Casimir force at a finite cut-off A by summing the forces induced by the all fluctuation modes. We show that the Casimir force is independent of the cut-off function in the limit L∧ → ∞. There is a correction in the order of （L∧）^-2, when L∧ is finite and large. This correction becomes remarkable when L is comparable with the microscopic length scale ∧^-1. It has been demonstrated that the Casimir force at a finite cut-off should be defined by summing forces of all fluctuation modes, instead of the derivative of Casimir energy with respect to L where an additional derivative of the cut-off function has been introduced.     

Casimir Force at a Finite Cut-Off

We calculate the Casimir force at a finite cut-off Λ by summing the forces induced by the all fluctuation modes. We show that the Casimir force is independent of the cut-off function in the limit LΛ → ∞. There is a correction in the order of (LΛ)^-2, when LΛ is finite and large. This correction becomes remarkable when L is comparable with the microscopic length scale Λ^-1. It has been demonstrated that the Casimir force at a finite cut-off should be defined by summing forces of all fluctuation modes, instead of the derivative of Casimir energy with respect to L where an additional derivative of the cut-off function has been introduced.