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研究了双模SU(1,1)相干态光场与V型三能级原子玻色-爱因斯坦凝聚(BEC)相互作用系统中光场的量子相关性质、振幅平方压缩效应和原子激光压缩效应。结果表明,双模SU(1,1)相干态光场各模的二阶相干度不随时间变化,光场各模光子是反聚束的,呈现非经典效应,光场两模相关性是非经典相关。光场具有周期性的振幅平方压缩效应,讨论了光场相关参数和原子相关参数对压缩深度、压缩频率的影响。双模原子激光不易压缩,压缩深度取决于光场初态。 相似文献
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利用SU(2)李代数讨论了原子相干态中角动量的二阶、四阶和六阶涨落,并在高阶不确定关系基础上提出了角动量高阶压缩的定义.研究了原子相干态中角动量涨落的二阶、四阶和六阶压缩情况.运用这里的定义和方法可进一步研究更高阶的压缩情况,从而把高阶压缩推广到原子算符的涨落上.
关键词:
原子相干态
Bloch态
SU(2)压缩 相似文献
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利用Raman相互作用制备双模SU(2)薛定谔猫态 总被引:1,自引:1,他引:0
首先将腔场制备成双模SU(2)态,然后不断注入与腔场发生Raman相互作用的V型三能级原子,通过原子一腔场相互作用生成腔场一原子纠缠,依次通过对原子进行选择性测量,利用波包塌缩原理,即可获得双模SU(2)场纠缠态。 相似文献
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利用一个参量频率转换过程,在腔中制备双模SU(2)相干态,然后注入A型三能级原子,使之与腔场的一个模发生Raman相互作用,生成腔场-原子纠缠态,通过对原子进行选择性测量,可获得奇偶SU(2)相干态.我们分别将原子能级和奇偶相干态编者按码为目标量子比特和控制量子比特,利用Raman相互作用可构造出类可控非门. 相似文献
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类Kerr介质中双模SU(1,1)相干态场与Λ型三能级原子相互作用的量子统计性质 总被引:1,自引:0,他引:1
导出了类Kerr介质中双模SU(1,1)相干态场与Λ型三能级原子相互作用系统的态函数,研究了Kerr效应对Λ型三能级原子布居概率、双模SU(1,1)相干态场的互关联函数、Cauchy-Schwartz不等式及二阶相干度的影响.结果表明:Kerr效应使原子与光场的耦合减弱,原子布居的崩塌与复苏的周期缩短;在初始光场较弱和较强两种情况下,类Kerr介质对双模SU(1,1)相干态场两模间的相关性、相关程度以及光子的聚束与反聚束效应产生的作用有明显的区别. 相似文献
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腔内混合态原子系统中辐射场的压缩效应 总被引:19,自引:2,他引:17
本文应用熵最大原理,假定腔内二能级原子起初就没有关于系统所处态的任何信息,研究了腔内原子与腔场相互作用的压缩行为,得出了原子初始处于任意统计混合态下,当初始激发足够强时,辐射场将产生极其接近于纯态情况在相同激发时的强压缩现象的重要结果,同时还讨论了产生压缩的混态范围。 相似文献
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与二项式光场相互作用的运动原子熵压缩 总被引:2,自引:2,他引:0
运用量子信息熵理论,研究了二项式光场与运动二能级原子相互作用过程中运动原子的信息熵压缩。讨论了不同的原子初态和场的有关参数对原子信息熵压缩的影响。结果表明:选择原子初态、场模结构、场调节参数及原子运动速度可以调控原子信息熵的压缩方向、偶极矩分量值和压缩周期;适当的选择参数可得到持续性的原子信息熵压缩。 相似文献
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Summary We have studied the squeezing properties of the atom and the radiation field in arbitrary intensity-dependent-coupling Jaynes-Cummings
model when it is restricted to the following initial condition: the atom in its coherent state and the field in the vacuum
state. The influence of virtual-photon processes on the atomic squeezing predicted by the Jaynes-Cummings model (JCM) has
been examined. The relationship between the field and atomic squeezing in the resonant multi-photon JCM has been discussed.
The symmetry between the field and atomic squeezing (SFAS) has been exposed in the resonant vacuum one-photon JCM, and the
influence of non-resonant interaction and virtual-photon processes on the SFAS has also been discussed. 相似文献
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The quadrature squeezing properties of an atom laser originating from atomic Bose-Einstein condensate interacting with light field are studied. We find that the squeezing properties of the atom laser are dependent on the initial light field interacting with the atomic Bose-Einstein condensate. If the initial light field cannot be squeezed, such as number state or coherent state light field, the atom laser as well cannot be squeezed. However, if the initial light field interacting with the atomic Bose-Einstein condensate being in squeezed state, the atom laser can be squeezed periodically, and its squeezing depth is dependent on the intensity of interatoms interaction. 相似文献
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利用一个参量频率转换过程,在腔中制备双模SU(2)相干态,然后注入一个与腔场的一个个模发生拉曼相互作用的A型三能级原子,通过原子-腔场相互作用生成腔场-原子纠缠,通过对原子进行选择性测量,腔场-原子纠缠态将塌缩到纯态,即双模SU(2)薛定谔猫态。 相似文献
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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
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
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采用全量子理论和数值计算方法,研究了初始处于SU(2)相干态的双模腔场与一个A型三能级原子共振相互作用的光场非经典性质,讨论了在没有对原子进行态选择测量、直接对原子进行态选择测量和应用经典微波场并对原子进行态选择测量的三种情况下,两个腔模总光子数、配分参量和耦合系数对光场非经典性质的影响.结果表明,增加两个腔模的总光子数M或对原子进行态选择测量,双模差压缩明显增强;减小配分参量和应用经典场并对原子进行态选择测量,α模光子的亚Poisson统计分布的平均程度变浅,而b模变深;两模间的反相关特征保持不变,增加M或直接对原子进行态选择测量,反相关平均程度变浅;直接对原子进行态选择测量,违背CauchySchwartz不等式.Abstract: Nonclassical properties of a two-mode field initially in an SU(2)coherent state resonantly interacting with a threelevel A-type atom are investigated by means of the quantum theory and numerical calculations.The dependence of the nonclassical properties on the total photon number of the two-mode,the partition parameter and the coupling constant is discussed for three cases:(1)no state-selective atomic measurement;(2)direct state-selective atomic measurement;and (3)state-selective atomic measurement after the application of a classical field.The results indicate that when the total photon number of the two-mode is increased or the state-selective measurement is performed on the atom,the difference squeezing of two-mode is distinctly enhanced;and when the partition parameter is decreased or the state-selective measurement is performed on the atom after the application of a classical field,the average intensity of the sub-Poisson statistic distribution of mode a is reduced and that of mode b is enhanced;when the total photon number of the two modes is increased or the direct state-selective measurement is performed on the atom,the anti-correlation character between the two modes is preserved,but the average intensity of the anti-correlation is reduced;and when the direct state-selective measurement is performed on the atom,the Cauchy-Schwartz inequality is violated. 相似文献
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