在Jaynes—Cummings模型中压缩真空初态场位相演化特性

应用Ｐｅｇｇ－Ｂａｒｎｅｔｔ位相理论，研究了Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ模型（Ｊ－Ｃ模型）中压缩真空初态场位相演化特性，具体计算了弱压缩条件下，场的位相几率分布函数及位相涨落，给出了在极坐标中位相几率分布演化曲线，讨论了原子与场相互作用对场的位相性质的影响。     

k（k〉2）光子Jaynes—Cummings模型中自发辐射场的位相演化特性

应用Ｐｅｇｇ－Ｂａｒｎｅｔ（ＰＢ）位相理论，研究了ｋ光子Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ（Ｊ－Ｃ）模型中自发辐射场的位相演化特性，计算了辐射场的位相几率分布函数与位相涨落，给出了在极坐标中位相几率分布演化曲线。     

双光子Jaynes—Cummings模型中的Schrodinger cat态

计算了双光子Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ模型场熵的演化，结合光子数统计分布和位相分布论证了双光子Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ模型在强场情况和某些特定时刻存在“Ｓｃｈｒｏｄｉｎｇｅｒ ｃａｔ”态的迭加态。     

q变形光场与两能级原子相互作用中场的位相特性

用变形Ｐｅｇｇ－Ｂａｒｎｅｔｔ位相理论研究了在共振情况下变形Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ（Ｊ－Ｃ）框或场的位相特性。讨论了ｑ变形参量对场位相统计和动力学性质 影响。     

附加克尔介质Jaynes－Cummings模型的场熵演化

研究了附加克尔（Ｋｅｒｒ）介质Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ（Ｊ－Ｃ）模型场熵演化的动力学特性，讨论了克尔介质非线性相互作用以及失谐量对场熵演化的影响．     

附加克尔介质Jaynes—Cummings模型的场熵演化

研究了附加克尔（Ｋｅｒｒ）介质Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ（Ｊ－Ｃ）模型场熵演化的动力学特性，讨论了克尔介质非线性相互作用以及失谐量对场熵演化的影响。     

非旋波近似下Jaynes—Cummings模型中的场熵演化

研究了非旋波近似下Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ（Ｊ－Ｃ）模型中的场熵演化规律，并与旋波近似下的相应结果进行比较，讨论了虚光子过程对场熵演化的影响。     

非旋波近似下Jaynes-Cummings模型中的场熵演化

研究了非旋波近似下Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ（Ｊ－Ｃ）模型中的场熵演化规律，并与旋波近似下的相应结果进行比较，讨论了虚光子过程对场熵演化的影响。     

论Jaynes—Cummings模型中原子偶极压缩和光场压缩间的关联

通过考察单光子Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇｓ（Ｊ－Ｃ）模型和非简并双光子Ｊ－Ｃ模型中原子偶极压缩和光场压缩随时间演化的规律，研究了原子偶极压缩与光场压缩之间的关系，给出了处于偶极压缩状态的原子辐射压缩光的条件，并讨论了原子压缩分量与光场压缩分量之间相互转化的特征，指出了原子－光场间的双光子耦合系统比单光子耦合系统更有利于制备压缩程度深的压缩光。     

原子相干性对光场振幅平方压缩的影响

研究了依赖型强度耦合Ｊａｙｎｅｓ－Ｃｕｍｍｉｎｇ模型中原子相干性对光场振幅平方压缩的影响，结果表明，光场振幅平方压缩效应依赖于原子的初态和原子与光场的相对位相角。     

压缩真空场与耦合双原子Raman相互作用过程中光场的相位演化特性

采用Pegg-Barnett相位理论，研究了压缩真空场与耦合双原子Raman相互作用过程中光场的相位演化特性.具体计算了场的相位概率分布函数及相位涨落，给出了在极坐标中概率分布变化曲线.讨论了原子与场相互作用、两原子间偶极-偶极相互作用以及原子初始状态对光场相位性质的影响. 关键词： 相位特性 压缩真空场 耦合双原子 Raman相互作用     

与压缩真空相互作用的具有强度耦合的广义Jaynes-Cummings模型的相位动力学

考虑具有强度耦合的广义Jaynes-Cummings模型与压缩真空相互作用.根据Pegg和Barnett新的相位理论,不仅得到了压缩真空场的相位分布,相位期待值和相位涨落的普遍表示式,及其演化图示,而且还导出了弱压缩真空和强压缩真空情形的近似角析表示式.对于压缩真空的压缩量与相位特性之间的关系进行了简要讨论.     

Phase properties of squeezed states of light

Recently introduced unitary and hermitian phase operators are used to examine the phase properties of squeezed states of light with particular reference to the squeezed vacuum. The results differ markedly from previous calculations involving the Susskind and Glogower operators. The new formalism allows the construction of a phase probability density which, on a polar diagram, is a circle for the vacuum state, becomes elliptical with gentle squeezing and collapses to a line through the origin for full squeezing. This probability density together with the calculation of expectation values of various trigonometrical functions of phase show how squeezing impresses phase information onto the vacuum.     

Properties of the q-Analogue of a Squeezed Vacuum State

We constructed a normalizable q-analogue of squeezed vacuum state using the technique of integration within an ordered product (IWOP) of operators and the properties of the inverses of q-deformed creation and annihilation operatots. We also study its nonclassical properties and phase probability distribution.     

Quantum phase distribution and the number—phase Wigner function of the generalized squeezed vacuum states associated with solvable quantum systems

The quantum phase properties of the generalized squeezed vacuum states associated with solvable quantum systems are studied by using the Pegg-Barnett formalism.Then,two nonclassical features,i.e.,squeezing in the number and phase operators,as well as the number-phase Wigner function of the generalized squeezed states are investigated.Due to some actual physical situations,the present approach is applied to two classes of generalized squeezed states:solvable quantum systems with discrete spectra and nonlinear squeezed states with particular nonlinear functions.Finally,the time evolution of the nonclassical properties of the considered systems has been numerically investigated.     

Phase properties of the nonlinear squeezed vacuum states

Using properties of the inverses of annihilation and creation operators of f-oscillator we construct the f-analogues of squeezed vacuum states. If used to describe the motion of a trapped ion, the phase probability distributions of these states for large η are very different from those of the usual squeezed vacuum state.     

铷原子D1线真空压缩光场的产生及态重构

碱金属原子是光量子存储的良好介质,与碱金属原子共振的非经典光场是量子信息处理的重要资源.本文采用周期极化磷酸氧钛晶体作为非线性介质,利用参量振荡过程产生了795 nm(铷原子D1线)的真空压缩光场.通过对平衡零拍探测系统的时域信号进行采集,得到压缩光场不同相位角下的噪声分布;利用极大似然估计法对压缩光场进行了态重构,得到了密度矩阵及相空间的Wigner函数.理论计算了真空压缩场的光子数分布和Wigner函数,并对理论计算结果和极大似然重构结果进行了分析和比较.     

Interaction of a Three-Level Atom and Field in a Squeezed Vacuum State with Added Photons: Quantum Phase and Nonclassical Properties

We present a detail study of the evolution of nonlocal correlations of an interacting quantum system comprising a three-level atom and a field mode initially prepared in a squeezed vacuum state with added photons. We compare the dynamical behavior of the quantum phase and entanglement by varying the number of photons added to the squeezed vacuum state. Furthermore, we examine the influence of the added-photon number and the squeeze parameter on the dynamical behavior of entanglement, quantum phase, and nonclassical properties of the field. Moreover, we explore the link between the quantum phase and the nonlocal correlation. Finally, we introduce an effective method to generate and maintain a high level of entanglement for this quantum system based on precise parameter ranges.     

激发压缩真空态的相位概率分布

应用Pegg和Barnett提出的相位算符和相位态理论,研究了激发压缩真空态的相位概率分布特性.数值计算结果表明,激发压缩真空态的相位概率分布主要受到相位参量和压缩参量的调节,相位参量使相位概率分布呈峰值结构,压缩参量的变化将影响相位概率分布的峰值强度,此外激发光子数对相位概率分布也有较大的影响.