与双模光场作用的Λ型三能级原子及其二能级近似

从多能级原子与多模光场的相互作用哈密顿量出发,导出了Λ型三能级原子与双模光场的相互作用哈密顿量。在大失谐条件下将其化成等效的二能级形式-双模喇曼耦合模型。提出了该模型的一个改进型等效哈密顿量。该哈密顿量由两部分构成:一部为通常所谓的等效哈密顿量,另一部分描述原子能级的动态斯塔克移动。研究表明,在双模喇曼耦合模型的研究中,只考虑前者是不够的,还必须考虑后者。最后,我们研究了该系统中原子的动力学行为,发现崩塌-复苏的数目、崩塌时间和复苏时间均呈现新的特性。     

与双模光场作用的Λ型三能级原子及其二能级近似

从多能级原子与多模光场的相互作用哈密顿量出发,导出了Λ型三能级原子与双模光场的相互作用哈密顿量．在大失谐条件下将其化成等效的二能级形式－双模喇曼耦合模型．提出了该模型的一个改进型等效哈密顿量．该哈密顿量由两部分构成：一部为通常所谓的等效哈密顿量,另一部分描述原子能级的动态斯塔克移动．研究表明,在双模喇曼耦合模型的研究中,只考虑前者是不够的,还必须考虑后者．最后,我们研究了该系统中原子的动力学行为,发现崩塌－复苏的数目、崩塌时间和复苏时间均呈现新的特性．     

非旋波近似下三能级哈密顿量的两能级简化

讨论旋波近似和非旋波近似两种条件下三能级系统哈密顿量的两能级简化及相关物理效应。     

双光子共振介质光学双稳特性的理论研究

本文给出了有关双光子共振介质中光学双稳的一般理论。分析了在双光子离共振和双光子近共振情形下的光学双稳特性,以及在双光子近共振情形时的瞬态光学双稳特性。在分析过程中建立和运用了双光子矢量模型。在数值计算的基础上作出了钠蒸汽中双光子共振附近情形下的光学双稳特性曲线。 关键词：     

非旋波近似下Ξ型三能级哈密顿量的两能级简化

讨论旋波近似和非旋波近似两种条件下Ξ型三能级系统哈密顿量的两能级简化及相关物理效应。     

双模量子腔场中两Λ型三能级原子的纠缠演化特性

本文采用Λ型三能级原子模型，其两个低能态之间的耦极跃迁是被禁戒的，考虑两个此种原子与一双模量子腔场的喇曼耦合模型，在双光子共振和单光子大失谐条件下，绝热消去了系统哈密顿量中原子的激发态，而研究两低能态间的纠缠。     

双光子光学双稳态的研究

用量子的方法,退关联近似,获得了三能级简并双光子双稳态方程。所得结果与实验相符合。指出用双光子矢量模型方法处理的缺点以及它与实验不符的原因。 关键词：     

在Kerr型介质中原子和场的性质

本文研究了在Ｋｅｒｒ型介质腔中经双光子辐射的二能级级联型原子和三能级级联型原子的动力学，在初始可干态下分别用有效效哈密顿量方法（含Ｓｔａｒｋ位移项）和全哈密顿量方法获得精确解，继而比较了原子的粒子数反转，光子统计分布，聚束与反聚束特性以及光场压缩性特性的数值结果，由此证明了在非线性介质的条件下，两种方法所获得结果类同，差异很小。     

UMSCTS中光子回波的研究

对级联三能级系统超快调制光谱学(UMSCTS)中的光子回波进行了研究.当宽带线宽且相对时延τ>0时单光子和双光子四波混频分别对应于三脉冲受激光子回波与和频三能级光子回波.宽带τ＜0时与窄带情形类似. 关键词：     

压缩真空中梯形三能级原子的辐射压力

研究了压缩真空中梯形三能级原子在单色行波场中的辐射压力。从系统的哈密顿量出发,利用玻因-马尔可夫近似,推导出了原子的光学布洛赫方程。此时用数值方法求得布洛赫方程的稳态解,然后用图示法考察了原子的辐射压力随双光子失谐、拉比频率、自发发射率等参量的依赖关系。结果表明：单光子跃迁和双光子跃迁可导致辐射压力出现各自的多普勒位移共振峰;辐射压力表现出较宽的失谐范围且强烈依赖于压缩参量以及压缩真空和相干光之间的相位关系。当相位满足匹配条件时,辐射压力减小。     

Quantum theory of optical multistability in a two-photon three-level medium

An effective Hamiltonian for the two-level model is derived from the microscopic Hamiltonian of a three-level atom in a configuration, interacting through two-photon transitions with a lightfield. The effective Hamiltonian includes a term describing the optical Stark shift. With this effective Hamiltonian, we study the steady-state equation and the squeezing spectrum from a cavity field mode interacting with an ensemble of three level configuration atoms by a two-photon transition. It is shown that the inclusion of optical Stark shift brings about changes in drift and diffusion coefficients as well as additional nonzero correlations between the stochastic forces. As a result, although qualitative features remain unaltered, quantitative changes both in the transmission characteristics and the squeezing spectrum are significant.     

Effective Raman Theory for a Three-Level Atom in the V-Configuration

It is shown that the system of a three-level atom coupled with two modes of quantized cavity fields in the V-configuration with arbitrary detunings can be exactly reduced to a two-level system with a nonsingular effective coupling which depends nonlinearly on the intensity of the two cavity fields. By performing a unitary transformation, we obtain an exact transformed Hamiltonian in which one of the three levels is decoupled for all values of the detunings including the zero-detuning. We also present the analytical expressions of energy eigenvdues and eigenvectors, evolution operator, time-varying atomic inversion operator and photon number operators of the two modes for the effective two-level model.     

Langevin and generalized Langevin types of spontaneous emission of quantum particles

In the effective Hamiltonian representation, we have obtained a quantum stochastic differential equation of a generalized Langevin type for the evolution operator of an atomic ensemble in a microcavity in an external broadband quantized field and in a nonresonant field of the microcavity. We show that, depending on the number of particles in the atomic ensemble, its dynamics demonstrates both the Langevin and the generalized Langevin types of the two-photon spontaneous decay. In this case, one photon is emitted into the cavity mode, whereas the other photon is emitted into the external broadband electromagnetic field. The Langevin type is determined by a considerable Stark interaction of the atomic ensemble with the broadband photon-free quantized field. We show that, here, the Stark interaction is represented by a quantized Poisson process and, depending on its magnitude (at certain numbers of atoms in the ensemble), the two-photon collective spontaneous emission of microcavity atoms can be completely suppressed. In this case, the two-photon spontaneous emission of the singly excited atomic ensemble is described by the two-level model, while the atom-photon cluster of the microcavity under the described conditions is an artificial two-level quantum particle with a strong Stark interaction.     

含非线性修正项的双光子Jaynes-Cummings模型中光子反聚束效应的研究

研究了一个二能级里德伯原子在计及原子散射的二级修正项时,与单模热光场双光子相互作用系统中光子的反聚束效应,着重讨论了非线性修正项,双光子失谐量以及热噪声对光子反聚束效应的影响． 关键词：     

Resonance Fluorescence in Two—Photon JC Models Analyzed by Supersymmetric Transformation

Resonance fluorescences of two-photon two-level and two-photon three-level atoms driven by laser are investigated with supersymmetric transformation.It is shown that the spectrum of fluorescent light obtained from the supersymmetric transformation is more accurate and the physical process shown by this method is clearer than that from dress transformation.     

Comment on ``Approximate and Conditional Teleportation of an Unknown Atomic State Without Bell-State Measurement with Two-Photon Interaction'

In a previous work [Commun. Theor. Phys. 45 (2006) 79] a scheme waspresented for approximate and conditional teleportation of an unknown atomicstate in a QED-cavity without Bell-state measurement via two-photonJaynes-Cummings model in the effective Hamiltonian approach. This commentpresents an alternative method, based on the so called ``full two-photonJaynes-Cummings Hamiltonian approach". Accordingly, it describes the evolution of the two-photon degenerate process for arbitrary average photon number inside the cavity, as the correct way to implement teleportation in this scenario.     

虚光场在原子的周期衰变和回复效应中的影响

本文利用非相对论量子电动力学理论,研究了在旋波近似(RWA)和非旋波近似下与双光子场作用的二能级原子算符的时间演化规律,通过数值法和解析法论证了虚光场是原子的周期衰变和回复呈现量子噪声的根源,并且说明了可忽略虚光场对回复时间影响的原因。     

Quantum Theory of a Nondegenerate Two-Photon Laser

Laser actions and photon statistics far a nondegenerate two-photon laser in an effective three-level stomic system with arbitrary detunlng are Investigated both semiclassically and quantum meehmleally, Due to the two-photon effect, the radiation field easily displays a sub-Foissonian statlstieal distribution. The laser actions for a two-photon and a sihgle-photon loss mechanisms are compared. It is found that the detailed balance in the single-photon loss mechanism can still be preserved in the case that a first-order phase transtion takes place.     

Dynamics of atom-field entanglement in a bimodal cavity

In this paper we investigate some aspects of the dynamics and entanglement of bipartite quantum system (atom-quantized field), coupled to a third “external” subsystem (quantized field). We make use of the Raman coupled model; a three-level atom in a lambda configuration interacting with two modes of the quantized cavity field. We consider the far off resonance limit, which allows the derivation of an effective Hamiltonian of a two-level atom coupled to the fields. We also make a comparison with the situation in which one of the modes is treated classically rather than prepared in a quantum field (coherent state).     

Influence of a Classical Homogeneous Gravitational Field on Dissipative Dynamics of the Phase Damped Jaynes–Cummings Model under the Markovian Approximation

In this paper, we study the dissipative dynamics of the phase damped Jaynes–Cummings model under the Markovian approximation in the presence of a classical homogeneous gravitational field. The model consists of a moving two-level atom simultaneously exposed to the gravitational field and a single-mode traveling radiation field in the presence of a phase damping mechanism. We first present the master equation for the reduced density operator of the system under the Markovian approximation in terms of a Hamiltonian describing the atom-field interaction in the presence of a homogeneous gravitational field. Then, by making use of the super-operator technique, we obtain an exact solution of the master equation. Assuming that initially the radiation field is prepared in a Glauber coherent state and the two-level atom is in the excited state, we investigate the influence of gravity on the temporal evolution of collapses and revivals of the atomic population inversion, atomic dipole squeezing, atomic momentum diffusion, photon counting statistics and quadrature squeezing of the radiation field in the presence of phase damping.