色散吸收一维光学系统中光场量子起伏的功率谱

利用格林函数方法量子化色散吸收介质中的电磁场,针对由三层色散吸收介质组成的一维光学系统,研究其中光场的量子理论,借助起伏一耗散定理给出色散吸收介质光腔中光场量子起伏的功率谱,并通过数值计算结果分析和讨论介质的色散吸收性质对光学器件工作性能的影响。结果表明,系统的工作状态与所选光场频率密切相关,并且每一区域中介质的色散吸收性不但影响自身区域的电场起伏功率谱,而且明显地连带另一侧介质中电场起伏功率谱的变化行为。此结果对于研究复杂的介质分布与结构体系在光通信、现代光学工程、微波技术等领域中的实际应用有着重要的指导意义。     

色散吸收非对称介质光腔系统中光场量子起伏的功率谱

借助系统格林函数和色散吸收介质中电磁场量子化过程,通过数值计算研究非对称色散吸收介质光腔系统中光场量子起伏的功率谱.结果表明,介质的折射和吸收性质分别对真空场起伏功率谱的振荡频率、振幅产生影响,腔两侧介质折射系数的对称性能更有效地抑制腔外空间场起伏功率谱的振荡;介质折射系数愈大,则其中光场起伏功率谱振荡中心愈低、振荡频率愈大,与此同时,光腔内真空场起伏功率谱振荡幅度加大.     

等离子体加载色散吸收对称介质光腔的量子理论

利用色散吸收介质中电磁场的正则量子化方法，研究等离子体加载对色散吸收介质光腔系统量子性质的影响。结果表明，介质加载使系统真空场起伏功率谐的空间分布发生明显变化。     

色散吸收非对称介质光腔中光场的量子理论

利用格林函数方法对色散吸收介质中的电磁场量子化,研究了由色散吸收介质构成的非对称介质光腔中光场的量子理论,并分析了非对称性对光腔量子性质、工作性能等的影响.     

非对称半导体量子阱中自发辐射相干诱导透明

研究了一束低强度探测脉冲光场在一个非对称半导体量子阱中的传输特性.在相同参数条件下,通过由自发辐射相干产生的交叉耦合系数来调控介质对探测场吸收、色散的变化规律.结果表明:从自发辐射相干的引入到达到相干最大,介质的吸收不断减小,同时强色散也随之进入透明窗口.     

经典光场相干控制金属纳米线表面等离子体传输

利用全量子力学的方法从理论上研究了利用经典光场相干控制半导体量子点-金属纳米线复合体系中表面等离子体传输特性. 计算中假设金属纳米线表面等离子体具有线性色散关系,半导体量子点具有梯形三能级结构. 分析表明:通过加或不加经典光场,可以控制表面等离子体被反射还是透射;加上光场后,反射峰、透射峰的位置以及两反射峰之间的距离都可以由经典光场控制. 关键词： 表面等离子体 量子点 散射     

非对称耦合量子阱吸收与色散的理论研究

基于V型三能级模型研究了非对称耦合量子阱（ACQW）线性吸收与色散特性. 理论结果表明：在小偏置区，由沿生长方向的外加电场引起的强量子限域Stark频移导致非共振吸收，线性折射率大幅度降低，表现为色散猝灭特性. 而随负偏压进一步增加, 由于量子限域Stark效应消失，其吸收与色散特性则与单量子阱最低激子态相类似. 这意味着ACQW具有随外加电场变化的可控色散特性. 关键词： 非对称耦合量子阱 量子相干 可控色散     

在V型系统中原子相干对吸收—色散关系的影响

在V型能级系统原子介质中,若利用外场产生相干,则弱光场在该介质中的吸收-色散关系将展现出新的特性.特别是当弱场具有某一特定频率时,介质对光的吸收为零但光折射率大于1.     

量子化电磁场在色散吸收有限介质中的传播

通过量子化吸收和色散介质中的电磁场,研究线极化波垂直入射至吸收和色散介质界面处的反射和折射行为,给出介质界面处光的正则量子理论.     

连续变量二类倍频过程中的量子信息操控

从Ⅱ类匹配倍频过程的半经典运动方程出发,讨论了阈值以下三共振Ⅱ类倍频过程中两个非简并基频光模为振幅压缩光场时产生的谐振倍频光场的量子起伏特性。通过对输入基频光场的振幅压缩调节来实现对倍频光场压缩度的控制。结果表明在这个系统中基频光场的量子起伏直接控制着倍频光场的量子起伏。这种以非线性过程实现的量子信息调控在量子通讯及量子网络中具有重要的意义。     

Influence of Quantum Effects on the Magnetic Field Behavior in Overdense Plasma

We study the conditions for the anomalous transmission of electromagnetic waves through quantum overdense plasma. We show that this anomalous transmission is triggered due to the excitation of surface waves, as was observed in the classical overdense plasma. The conditions for the excitation of surface waves are obtained by studying the dispersion relation within the framework of quantum hydrodynamics. The corresponding consequences at the classical limits are consistent with the previous studies. In comparison with the classical regimes, the quantum dispersion curve exhibits an asymptotic behavior which indicates significant effects, in particular, at large wavelengths. Herein, to create the required evanescent waves, we consider the quantum plasma to be placed between two ordinary prisms and dielectrics. The effects of the main parameters, such as the permittivity of the prisms and dielectrics and the Fermi velocity, on the rate of the transmission and the magnetic field propagation are also evaluated.     

Two-pulse correlations in noisy quantum channels

The modification of initially entangled light pulses passing through noisy quantum channels, modeled by dispersive and absorbing four-port devices, is studied with the help of recently obtained results on quantum state transformations. The fidelity and indices of quantum correlations based on the von Neumann entropy are calculated. Their dependence on both the pulse shape and the four-port device parameters is studied. It is shown that due to dispersion and absorption, the quantum correlations are reduced, and they decrease with increasing initial entanglement.     

Quantization of the radiation field in an anisotropic dielectric medium

There are both loss and dispersion characteristics for most dielectric media. In quantum theory the loss in medium is generally described by Langevin force in the Langevin noise (LN) scheme by which the quantization of the radiation field in various homogeneous absorbing dielectrics can be successfully actualized. However, it is invalid for the anisotropic dispersion medium. This paper extends the LN theory to an anisotropic dispersion medium and presented the quantization of the radiation field as well as the transformation relation between the homogeneous and anisotropic dispersion media.     

Transmissivity and reflectivity of spatially dispersive thin films

We calculate the transmission and reflection coefficients for electromagnetic radiation incident normally on the surfaces of thin, spatially dispersive, absorbing, dielectric films. Results are obtained for four models of spatially dispersive dielectrics and for the case in which spatial dispersion is neglected. For each model the effects of spatial dispersion are to introduce additional fine structure into the transmission and reflection coefficients, regarded either as functions of frequency or of the thickness of the film. In addition, the results reveal an interleaving between the maxima and minima of the spectra for different models, which may provide a basis for an experimental discrimination between different phenomenological models for the nonlocal dielectric constant of a spatially dispersive dielectric medium.     

Controlling the probe-absorption and -dispersion via quantum interference from incoherent pumping field in a four-level lambda-type system

Absorptive and dispersive properties of a four-level Λ-type atomic system with two fold lower levels are investigated. The effect of quantum interference induced by incoherent pump and spontaneous emission upon the absorption, dispersion, and group index is them discussed. In addition, the rate of an incoherent pump field and the intensity of coupling field on light propagation is also presented.     

一种适用于任意阶空间差分时域有限差分方法的色散介质通用吸收边界条件算法

基于伸展坐标完全匹配层方程和辅助微分方程 方法, 给出了一种在时域有限差分(FDTD) 计算中适用于常见色散介质的通用边界条件算法. 该算法适用于任意阶的FDTD空间差分, 并且由于所采用的D-H方程独立于计算区域, 所以可以被用于截断任意电介质. 数值试验结果表明, 与卷积完全匹配层 算法相比较, 所提出的吸收边界条件算法不仅通用性强、 计算复杂度低、 计算时间短, 并且吸收效果有明显的提高.     

Magneto-optical Faraday effects in dispersive properties for three-dimensional magnetized plasma photonic crystals

The dispersive properties of three-dimensional magnetized plasma photonic crystals composed of homogeneous magnetized plasma spheres immersed in isotropic dielectric host with face-centered-cubic lattices are theoretically studied based on plane wave expansion method, as the magneto-optical Faraday effects of magnetized plasma are considered. The equations for calculating the band structures are theoretically deduced. The photonic band gap and a flatbands region can be obtained. The influences of host dielectric constant, plasma collision frequency, filling factor, external magnetic field and plasma frequency on the dispersive properties are investigated in detail, respectively, and some corresponding physical explanations are also given. The numerical results show that the photonic band gap can be manipulated by the plasma frequency, filling factor, external magnetic field and host dielectric constant, respectively. However, the plasma collision frequency has no effects on photonic band gap. The location of flatbands region cannot be tuned by any parameters except for the plasma frequency and external magnetic field.