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1.
简并多光子过程中两能级原子消相干性的消除   总被引:6,自引:1,他引:5  
张登玉 《光子学报》2002,31(5):537-540
研究置于外部环境(热库)中的两能级原子消相干性的消除.在相互作用系统中通过外加驱动场的方法,得到简并多光子过程中两能级原子约化密度算符非对角元.当外加驱动场的演化规律满足一定的条件时,可使两能级原子的消相干被消除.  相似文献   

2.
张登玉 《光子学报》2003,32(6):762-764
两能级原子被嵌制在一充满类Kerr介质的热库中,通过求解原子与外加驱动场相互作用时约化密度算符非对角元,研究简并双光子过程中原子在外界环境(类Kerr介质和热库)下的相干特性.结果表明:当原子的相干性被保持时,外加驱动场的时间演化与原子的跃迁频率、原子偶极矩和模平均光子数等因素有关.  相似文献   

3.
消除热库中量子位的消相干性   总被引:4,自引:1,他引:3       下载免费PDF全文
以二能级原子作为量子位,利用求解相互作用系统约化密度矩阵非对角元的方法,分别研究热库中量子位模型和依赖强度耦合Jaynes-Cummings模型的消相干特性.当外加驱动场消除消相干时,得到两种模型下驱动场必须满足的约束方程.?  相似文献   

4.
谭荣  李高翔 《物理学报》2005,54(5):2059-2065
研究了处于三维光子晶体中,且在强相干的低频场的驱动下的单个二能级原子的自发辐射性质.由于低频场的影响,使得原子产生了在跃迁过程中吸收或发射一个低频光子的衰减渠道.这些跃迁导致了自发辐射的量子干涉,再加上光子晶体能带带边的作用,自发辐射被显著抑制.原子的布居俘获依赖于原子上能级与能带带边的相对位置,低频场的频率和原子不同跃迁通道间的相对跃迁强度. 关键词: 光子晶体 二能级原子 自发辐射  相似文献   

5.
利用投影算符技巧从刘维方程出发导出了二能级原子约化密度算符主方程,研究了压缩真空库场中二能级原子的非简并双光子荧光谱特性.发现与真空库或热库中双光子荧光不同,在非简并双光子情况中存在一种新型振荡现象,它具有上下两个阈值,在上下阈值之间原子发生振荡,在两阈值之外原子将不发生振荡.在两阈值之间原子的非简并双光子荧光谱呈现正峰结构,在两阈值之外双光子荧光谱具有负的峰结构.光谱形状强烈地依赖于双光子自然线宽,但光谱是非相敏性的,这是未曾预料到的. 关键词:  相似文献   

6.
章国顺  曹卓良 《光学学报》2008,28(8):1611-1617
采用时间演化算符方法,研究∧-型=三能级原子与纠缠相干态光场共振相互作用的辐射谱.给出了辐射谱一般公式,并讨论在纠缠相干态光场驱动下的辐射频谱结构.结果表明,无论下能级简并与否纠缠相干态光场平均光子数很小时均出现拉比分裂,且强度随双模光场纠缠程度的增加而增加.当两下能级简并时,若两模场的平均光子数较小,辐射谱呈现对称多峰结构,若两模场的平均光子数较大,辐射谱呈现对称五峰结构.当两下能级非简并时,若两模场的平均光子数较小,辐射谱呈现对称多峰结构.若两模场的平均光子数较大,辐射谱呈现对称十峰结构.纠缠相干光与非纠缠相干光辐射谱的本质差别有两点:一是双模光场强量子关联导致纠缠度越强拉比峰强度越高;二是存在纠缠时由于两模场相干性导致辐射谱呈现对称多峰结构.  相似文献   

7.
SU(2)相干态场与二能级原子的非简并双光子相互作用   总被引:5,自引:0,他引:5  
路洪  彭金牛 《光学学报》1995,15(10):365-1370
研究了双模SU(2)相干态场与腔中二能级原子的非简并双光子相互作用。用数值计算讨论了SU(2)光场的反关联特性对原子动力学行的影响及场的量子统计性质时间的演化。  相似文献   

8.
田永红  彭金生 《物理学报》1999,48(11):2060-2069
运用全量子理论研究了双模压缩真空场与二能级原子双光子作用过程中原子的量子行为,论证了原子发生相干俘获的条件,讨论了压缩参数对原子偶极压缩的影响. 关键词:  相似文献   

9.
为了研究三光子过程中原子与相干态耦合量子体系信息熵压缩随时间演化规律及原子最佳信息熵压缩态的制备,我们采用全量子理论,推导出运动原子与单模简并三光子依赖强度耦合量子体系的精确解;理论上给出制备原子最佳信息熵压缩态的充分及必要条件,并进行了数值模拟验证.研究结果表明:控制相干态场与原子作用时间,切断相干态场与原子的纠缠,选择二能级原子处于等权重相干叠加态,适当选取相干态场与原子的初始位相,可以制备出原子最佳量子信息熵压缩态;调节光腔中场模结构参量,能够得到连续的量子信息熵压缩态.该研究结果在多光子过程低噪声量子信息处理中具有一定意义.  相似文献   

10.
根据简并Λ型三能级原子与单模光场的改进型有效哈密顿量 ,通过矩阵形式法推导出原子光场系统的波函数 ,提出利用简并Λ型三能级原子与单模光场的远离共振相互作用制备四光子相干态的有效方案。并且证明按照同样的方法不能制备出四成分以上的相干叠加态 ,即当在腔中注入的第三个原子的速度与第二个原子的速度相等时 ,腔场将保持这种四光子相干叠加态不变  相似文献   

11.
钱懿  许晶波 《中国物理 B》2012,21(3):30305-030305
We investigate a two-level atom interacting with a quantized cavity field and a classical driving field in the presence of phase decoherence and find that a stationary quantum discord can arise in the interaction of the atom and cavity field as the time turns to infinity. We also find that the stationary quantum discord can be increased by applying a classical driving field. Furthermore, we explore the quantum discord dynamics of two identical non-interacting two-level atoms independently interacting with a quantized cavity field and a classical driving field in the presence of phase decoherence. Results show that the quantum discord between two atoms is more robust than entanglement under phase decoherence and the classical driving field can help to improve the amount of quantum discord of the two atoms.  相似文献   

12.
We investigate a two-level atom interacting with a quantized cavity field and a classical driving field in the presence of phase decoherence and find that a stationary quantum discord can arise in the interaction of the atom and cavity field as the time turns to infinity.We also find that the stationary quantum discord can be increased by applying a classical driving field.Furthermore,we explore the quantum discord dynamics of two identical non-interacting two-level atoms independently interacting with a quantized cavity field and a classical driving field in the presence of phase decoherence.Results show that the quantum discord between two atoms is more robust than entanglement under phase decoherence and the classical driving field can help to improve the amount of quantum discord of the two atoms.  相似文献   

13.
两能级原子与外部环境(热库)相互作用时,采用非旋波近似,研究原子与热辐射场单光子和双光子作用过程,利用小系统与库耦合行为的量子理论,计算原子约化密度矩阵非对角元,分析原子状态的消相干特性。  相似文献   

14.
We consider an inertial two-level atom in interaction with a real massless scalar quantum field in a spacetime between two parallel reflecting plane boundaries, and calculate the contributions of vacuum fluctuations and radiation reaction to the rate of change of the atomic energy. Our results show that there exists a regime of the separation L between the two boundaries such that the excited atom's spontaneous emission is impossible. There also exist certain values of the atom's position such that the corrections due to the presence of boundaries balance each other, so that the atom's spontaneous emission rate is the same as if there were no boundaries at all.  相似文献   

15.
We present the exact solution of the dynamics of N two-level atoms strongly driven by an external coherent field and equally coupled on resonance to a cavity mode, in the presence of both cavity dissipation and atomic decay. Analytical results are presented for system and subsystem dynamics, showing how environment-induced decoherence leads the system from pure to mixed states. In the limit of negligible atomic decay, where the system is known to exhibit decoherence-free subspaces, we present a detailed discussion of the decoherence function that can be monitored by atomic population measurements.  相似文献   

16.
Solid-state qubits have the potential for the large-scale integration and for the flexibility of layout for quantum computing. However, their short decoherence time due to the coupling to the environment remains an important problem to be overcome. We propose a new superconducting qubit which incorporates a spin-electronic device: the qubit consists of a superconducting ring with a ferromagnetic pi junction which has a metallic contact and a normal Josephson junction with an insulating barrier. Thus, a quantum coherent two-level state is formed without an external magnetic field. This feature and the simple structure of the qubit make it possible to reduce its size leading to a long decoherence time.  相似文献   

17.
张剑  邵彬  邹健 《中国物理 B》2009,18(4):1517-1527
In this paper, we investigate the entropy squeezing for a two-level atom interacting with two quantized fields through Raman coupling. We obtain the dynamical evolution of the total system under the influence of intrinsic decoherence when the two quantized fields are prepared in a two-mode squeezing vacuum state initially. The effects of the field squeezing factor, the two-level atomic transition frequency, the second field frequency and the intrinsic decoherence on the entropy squeezing are discussed. Without intrinsic decoherence, the increase of field squeezing factor can break the entropy squeezing. The two-level atomic transition frequency changes only the period of oscillation but not the strength of entropy squeezing. The influence of the second field frequency is complicated. With the intrinsic decoherence taken into consideration, the results show that the stronger the intrinsic decoherence is, the more quickly the entropy squeezing will disappear. The increase of the atomic transition frequency can hasten the disappearance of entropy squeezing.  相似文献   

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