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 共查询到17条相似文献,搜索用时 78 毫秒
1.
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。  相似文献   

2.
色散吸收非对称介质光腔系统中光场量子起伏的功率谱   总被引:4,自引:1,他引:3  
崔元顺  周淮玲  付浩 《光子学报》2002,31(11):1312-1316
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.  相似文献   

3.
李明  崔元顺  陆建 《光学学报》2005,25(12):702-1706
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。  相似文献   

4.
量子化电磁场在色散吸收有限介质中的传播   总被引:8,自引:3,他引:5  
崔元顺 《光子学报》2000,29(7):577-582
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.  相似文献   

5.
崔元顺 《光子学报》2005,34(4):636-640
利用格林函数方法量子化色散吸收介质中的电磁场,研究了等离子体/色散吸收介质系统光场的量子性质.理论和数值计算表明,系统的工作状态与所选光场频率密切相关,等离子体介质的阻尼性明显地影响自身区域电场量子起伏功率谱,并且对另一侧介质中电场量子起伏功率谱的变化有连带作用.  相似文献   

6.
正交模分裂(或真空Rabi分裂)是原子与光学腔构成的复合系统实现强相互作用的一个典型现象.本文理论研究了三能级原子介质与腔构成的复合系统,利用线性色散理论将腔内三能级原子自感应透明(EIT)介质的吸收和色散引入光学腔透射公式,非常直观清晰得到腔透射谱的三个分裂峰,它是由腔内EIT介质的吸收和色散特性使一个共振腔模分裂为三个腔模.该方法可以推广到腔内含有任意色散和吸收的介质.  相似文献   

7.
一维对称光子晶体的简正耦合模   总被引:3,自引:3,他引:0       下载免费PDF全文
对一维对称光子晶体中的色散介质采用洛仑兹振子模型,通过考虑色散介质层两侧的边界条件,得到了表征色散介质层的转移矩阵.对线性层及色散δ层均采用传输矩阵的方法,研究了一维含色散介质的光子晶体微腔中的简正耦合模.由于光与色散介质的相互作用,纵腔模将分裂成简正耦合模.通过改变色散介质的相关参数,详细研究了简正耦合模频率的移动、均匀展宽效应和失谐效应.发现两个简正的耦合模的频率间距主要依赖于振子的耦合强度,与约化的振子的HWHM线宽无关.失谐效应则会使其中的一个峰降低,而另一个峰相对拉高,这一现象可以通过Fabry-Pérot腔得到很好的解释.  相似文献   

8.
用一种新提出的通用非线性光脉冲传输的量子理论,我们研究了具有啁啾的光脉冲在正色散克尔介质中传输时的压缩比变化情况,数值结果表明,正色散克尔介质中,光脉冲还是压缩态,但压缩和负色散克尔介质比起来弱一点,初始的负啁啾有利于压缩。  相似文献   

9.
研究了含色散介质的一维光子晶体微腔的透射谱,对色散介质采用Lorentz振子模型,腔模的频率设置在光子晶体带隙中心。发现当吸收可以忽略时,色散效应将导致在腔模附近有很高的态密度,与此相应地在透射谱中出现一个较宽的透射带。当吸收存在时透射带中心的透射峰消失,但带尾的透射峰依然存在。  相似文献   

10.
关于介质吸收与色散的振子特性参数   总被引:2,自引:0,他引:2  
根据共振模型,讨论影响介质的吸收与色散的振子特性参数,得到关于振子阻尼系数的振子数的解析式。据此,利用介质的吸收谱曲线可以定量计算振子的阻尼系数和振子数,这对研究和改善介质的吸收和色散特性有重要意义。我们已用此方法研究气液浓度的光电特性。  相似文献   

11.
李维  刘世炳  杨巍 《中国物理 B》2009,18(6):2314-2318
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.  相似文献   

12.
We propose an engineered reservoir inducing the relaxation of a cavity field towards nonclassical states. It is made up of two-level atoms crossing the cavity one at a time. Each atom-cavity interaction is first dispersive, then resonant, then dispersive again. The reservoir pointer states are those produced by an effective Kerr Hamiltonian acting on a coherent field. We thereby stabilize squeezed states and quantum superpositions of multiple coherent components in a cavity having a finite damping time. This robust decoherence protection method could be implemented in state-of-the-art experiments.  相似文献   

13.
A Rydberg atom coupled to a single field mode in a high Q superconducting cavity is an ideal tool to perform experiments testing the most puzzling aspects of the quantum theory. The coupling between the atom and the field is either resonant or dispersive. In the resonant case, quantum Rabi oscillations in the vacuum or in a small coherent field injected in the cavity are observed. The analysis of these signals reveals in a striking way the quantization of the field. Quantum Rabi oscillations are also used to produce entanglement between successive atoms crossing the cavity. Dispersive atom-field coupling is used to prepare coherent superpositions of field states with different phases (Schrödinger cat states). The progressive decoherence of these states is studied by measuring correlations between the energies of pairs of atoms sent through the cavity with a variable delay between them. These experiments provide fundamental tests of quantum theory and shed light on the transition from quantum to classical in mesoscopic systems.  相似文献   

14.
郑仕标 《中国物理》2003,12(1):51-54
We propose a quantum nondemolition measurement of the photon-number distribution for a weak eavity field with no more than two photons ,the scheme is based on the resonant interaction of atoms with the cavity field,and thus the required interaction time is much shorter than that using dispersive interaction.This is important in view of decoherence,Our shceme can also be used to generate even and odd coherent states for a weak cavity field with resonant atoms.  相似文献   

15.
本文提出了一个基于腔QED的隐形传送四比特团簇类态方案,在该方案中选用两个GHZ纠缠对作为量子通道,通过对原子和腔场的大失谐作用以及外加强经典场的辅助,可以制备纠缠的量子通道,完成联合的三粒子测量,成功地实现隐形传送四比特团簇类态。结果还表明,此方案不受腔场退相干和热场的影响.  相似文献   

16.
The rate of spontaneous emission of an atom in the presence of an interface between two dielectrics was calculated using the quantum theory of electromagnetic radiation. Spatial distribution of the field for quasi-continuous spectrum inside an infinite cavity with ideally conducting walls was determined for multiple values of real refractive indices. Spontaneous emission in the continuous spectrum of the field was calculated using the known spatial Green’s function for a one-dimensional dielectric interface. The rate of spontaneous emission of an atom may either be higher or much lower than that in the free space, depending on the refractive indices and the distance between the atom and the interface between dielectrics.  相似文献   

17.
A numerical analysis of dispersive quantum nondemolition measurement of the photon number of a microwave cavity field is presented. Simulations show that a key property of the dispersive atom-field interaction used in Ramsey interferometry is the extremely high sensitivity of the dynamics of atomic and field states to basic parameters of the system. When a monokinetic atomic beam is sent through a microwave cavity, a qualitative change in the field state can be caused by an uncontrollably small deviation of parameters (such as atom path length through the cavity, atom velocity, cavity mode frequency detuning, or atom-field coupling constants). The resulting cavity field can be either in a Fock state or in a super-Poissonian state (characterized by a large photon-number variance). When the atoms have a random velocity spread, the field is squeezed to a Fock state for arbitrary values of the system’s parameters. However, this makes detection of Ramsey fringes impossible, because the probability of detecting an atom in the upper or lower electronic state becomes a random quantity almost uniformly distributed over the interval between zero and unity, irrespective of the cavity photon number.  相似文献   

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