共查询到17条相似文献,搜索用时 156 毫秒
1.
根据Pegg-Barnett位相定义, 计算了一种新的奇偶非线性相干态的位相概率分布函数, 利用数值计算方法研究了它们的位相统计性质. 数值计算结果表明:新的奇偶非线性相干态的位相特性与通常奇偶相干态的位相特性截然不同. 相似文献
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相干态光场的位相统计性质 总被引:5,自引:0,他引:5
根据Pegg-Barnett位相定义,计算了相干态光场的位相概率分布函数,并且进行了数值模拟。研究表明在真空态时,位相分布曲线为一条直线;相干态下位相分布曲线表现为:均匀分布→泊松分布→均匀分布。 相似文献
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利用f-谐振子的产生和湮灭算符的逆算符,构造了两个非线性压缩单光子态,并借助于Pegg—Barnett位相算符公式和数值计算方法,研究了它们的位相概率分布。结果表明,两个非线性压缩单光子态的位相概率分布不同;与通常的压缩单光子态、非线性压缩真空态不同,在这两个非线性压缩单光子态中,其位相概率分布能明显地反映出不同的量子位相信息和干涉特性。 相似文献
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构造出了一种新的奇偶非线性相干态, 并借助于数值计算方法研究了它们的压缩、振幅平方压缩、反聚束和相位概率分布等非经典性质. 结果表明, 与通常的奇偶相干态和非线性奇偶相干态不同, 在参数|λ|的不同取值范围内, 新的奇偶非线性相干态在Y1和Y2两个方向均可呈现振幅平方压缩效应, 而压缩效应仅在偶非线性相干态的X2方向上呈现, 反聚束效应仅在奇非线性相干态中呈现. 另外, 通过研究新的奇偶非线性相干态相位概率分布, 发现新的奇偶非线性相干态具有完全不同的量子干涉特性.
关键词:
新的奇偶非线性相干态
压缩效应
反聚束
相位概率分布 相似文献
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附加克尔介质Jaynes—Cummings模型场的位相特性 总被引:3,自引:1,他引:2
运用Pegg-Barnett厄米位相公式,研究了附加克尔(Kerr)介质Jaynes-Cummings(J-C)模型场的位相特性.具体讨论了场的位相概率分布、厄米位相算符的期待值以及位相的涨落,通过与标准J-C模型作比较,讨论了克尔介质与模场的非线性相互作用对场位相特性的影响. 相似文献
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根据Pegg-Barnett 相位定义,计算了一种新的非线性叠加相干态的相位概率分布函数和光子数-相位压缩效应,并进行了数值模拟. 相似文献
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领头项相干态的PB位相统计性质 总被引:4,自引:1,他引:3
使用文献中给出的计算量子位相统计性质的方法计算了m取不同值时各领头相干态│a,m〉的量子位相统计性质,揭示出m和场强│a│这两个因素怎样影响│a,m〉的量子位相统计性质的,发现领头项相干态│a,m〉在场强│a│^2最接近m值时最好的相统计性质,从而加深了我们对相干态量子位相的性质和物理本质的理解。 相似文献
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构造出了有限维Hilbert空间Roy型奇偶非线性相干态, 讨论了它们的正交归一完备性和振幅平方压缩效应. 研究表明, 在此空间中Roy型奇偶非线性相干态是归一完备的, 但不具有正交性; 当复参数相位角θ满足一定条件时它们存在振幅平方压缩效应, 同时导出了压缩条件与参数s,r以及函数f(n)之间的关系. 最后借助于数值计算, 发现对于5维(或7维)Hilbert空间中Roy型偶(或奇)非线性相干态, 当参数θ和Lamb-Dike参数η取某一给定值时, 在参数r变化的不同取值范围内, 它们均可以呈现振幅平方
关键词:
有限维Hilbert空间
Roy型非线性相干态
奇偶非线性相干态
振幅平方压缩 相似文献
12.
Ji-Suo Wang Tang-Kun Liu Jian Feng Jin-Zuo Sun Ming-Sheng Zhan 《International Journal of Theoretical Physics》2003,42(12):2855-2862
Using the Pegg–Barnett formalism of phase operator, we obtain phase probability distributions of new even and odd nonlinear coherent states. It is shown that the distributions for the states are rather different, and unlike the case of ordinary even and odd coherent states the Pegg–Barnett distribution clearly reflects the different character of quantum interference in the case of the new even and odd coherent states. 相似文献
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Using a numerical computational method, quasiprobability distributions
of new kinds of even and odd nonlinear coherent states (EONLCS) are
investigated. The results show that the distributions of the new
even nonlinear coherent states (NLCS) are distinct from those of the new
odd NLCS and imply that the new EONLCS always exhibit some different
nonclassical effects. Finally, with the aid of newly introduced
intermediate coordinate-momentum representation in quantum optics,
the tomograms of the new EONLCS are calculated. This is a new way of
obtaining the tomogram function. 相似文献
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A new kind of k-quantum nonlinear coherent states, i.e., the k eigenstates of the
k-th power $\hat{B}^{k}$ (k≥3) of the
generalized annihilation operator $\hat{B}=\hat{a}\frac1{f(\hat{N})}$
of f-oscillators, are obtained and their properties are discussed.
The completeness of the k states is investigated. An alternative
method to construct them is proposed. It is shown that these states
may form a complete Hilbert space, and all of them can be generated by
a linear superposition of k Roy-type nonlinear coherent states.
Physically, they can be generated by a linear superposition of the
time-dependent Roy-type nonlinear coherent states at different
instants. 相似文献
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A new kind of even and odd nonlinear coherent states (EONLCSs) is introduced. Using the Pegg-Barnett formalism of phase operator we study the phase probability distributions of the new kind of EONLCSs. The numerical computation results show that the phase probability distributions for the new EONLCSs can clearly exhibit the different features of quantum interference and distinct from those of the ordinary even and odd coherent states (EOCSs) and EONLCSs. Based on the phase probability distributions we investigate the phase and number squeezing of the new EONLCSs. It is found that these states exhibit number squeezing for different ranges of the parameter |λ|. 相似文献
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Finite-dimensional even and odd nonlinear pair coherent states and their some nonclassical properties 下载免费PDF全文
In this paper a new class of finite-dimensional even and odd nonlinear pair coherent states (EONLPCSs), which can be realized via operating the superposed evolution operators D±(τ) on the state |q, 0), is constructed, then their orthonormalized property, completeness relations and some nonclassical properties are discussed. It is shown that the finite-dimensional EONLPCSs possess normalization and completeness relations. Moreover, the finite-dimensional EONLPCSs exhibit remarkably different sub-Poissonian distributions and phase probability distributions for different values of parameters q, η and ξ. 相似文献