利用原子-腔场喇曼相互作用制备纠缠压缩真空态

提出了利用量子态腔场与原子的喇曼相互作用制备纠缠压缩真空态的方案.在该方案中,一个初始制备在基态的原子被依次送入几个初始制备在压缩真空态的微腔中.通过控制原子的运行速度,使原子与每一个腔具有相同的相互作用时间.当原子与腔场发生相互作用,原子与腔场产生纠缠之后,进行原子的测量.当原子被测量处于基态或激发态时,按照量子力学波包塌缩原理,腔场态将塌缩到相应的纠缠压缩真空态.对纠缠压缩真空态的纠缠性质也进行了简略的讨论.     

双模腔场与一个V型三能级原子共振相互作用的压缩特性

采用全量子理论和数值计算方法,研究了初始处于相干态的双模腔场与一个V型三能级原子共振相互作用的压缩特性,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,腔模平均光子数、耦合系数以及相互作用时间对压缩特性的影响。证明了压缩随着两个腔模光子数的增加而增加,而且通过对原子进行态选择性测量可以使压缩大大地增强,即使少光子数也一样。综合所有情形,发现最大压缩可以接近75%。     

两原子双光子Jaynes-Cummings模型的腔场谱

研究了两个偶极相互作用二能级原子与高Q腔场双光子相互作用的腔场谱.给出了初始光场为Fock态、相干态和压缩真空态时的计算结果并解释了谱结构的形成,分析了原子间的偶极相互作用和初态的交换对称性对腔场谱的影响.发现当两原子均处于激发态时,腔场谱只在初始光场为真空态时出现4峰结构,而在其它初始场时,都呈现出奇数峰,这与相应的辐射谱偶数峰的结构明显不同.而两原子只有一个处于激发态时,腔场谱结构主要由原子初态是否具有交换对称性决定. 关键词：     

非等同两原子与双模叠加态腔场的拉曼相互作用

研究了处于双模腔中的两个非等同二能级原子与叠加态光场的拉曼相互作用,推导出了两模光场均处于光子数态和任意叠加态时腔场谱的计算公式,给出了两模初始场为相干态和压缩真空态时谱结构的数值结果,讨论了相对耦合常数R=g2/g1和初始场强对腔场谱的影响.发现腔场谱结构不仅与初始场强有关,还随初始场光子数分布的变化而改变.     

利用双通道级联型原子库实现辐射场双模压缩真空态

本文研究了利用双级联型四能级原子实现高纯度、强的双模腔场压缩纠缠态。考虑将四能级联型原子注入至一个双模腔中,腔场与原子能级形成共振的相互作用。在原子-腔场弱相互作用下,若原子自发辐射速率远大于腔场的衰减速率,在腔场相干时间内将原子视为腔场的外部环境库,我们推导出腔场所满足的主方程。通过分析主方程并发现:在不考虑腔场真空耗散的情况下,腔场等效地与一个双模压缩真空库耦合,因此在稳态区域处于纯的双模压缩真空态,并且压缩程度只依赖于原子初始上能级的布居;在考虑腔场耗散的情况下,耗散对其纯度的影响大于对纠缠的影响;与单通道原子库情况比较,利用双通道的原子库可以有效地提高腔场的纠缠和纯度。     

操作腔外原子可控制腔内原子的压缩特性

原子偶极压缩效应的研究一直是量子光学领域中的一个十分活跃的课题,而且这些研究中多限于初始处于单原子的单态或叠加态、双原子的直积态或相干态与光场的相互作用.近年来,原子的纠缠态引起了人们极大的研究兴趣.因为纠缠态不仅证明了量子力学的非局域性,而且被广泛应用于量子计算、量子密码术、量子隐形传态等方面.最近, Yang等人研究了初始处于EPR态的两个两能级原子,其中一个注入真空态腔中,然后通过对腔外原子的操作可以控制腔内原子的发射性质.Lin等人考虑了初始处于GHZ态的三个两能级原子,让其中两个原子分别注入两个处于真空态的共振腔中.在本文中,我们分别考虑原子初始处于EPR态或GHZ态,将其中一个或两个原子同时注入一个处于相干态的光腔中,在共振条件下通过操纵腔外原子来研究腔内原子的偶极压缩效应.结果表明:对腔外原子执行一次旋转操纵和测量,可以改变腔内原子存在的偶极压缩特性.这方面的研究工作对量子态的制备和腔场的辐射控制具有一定的实际意义.     

腔内混合态原子系统中辐射场的压缩效应

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。     

腔场初始态对两量子比特空间退相干的影响

研究了两个二能级原子与一个单模腔场的相互作用中,腔场的不同初始态对原子间相对位置退相干的影响。从描述原子间相对位置状态的约化密度矩阵出发,假设原子间相对位置为两个高斯波包的叠加态,讨论了当腔场初始态分别为热态、Fock态和压缩态情况下,原子与光场的相互作用对两原子间相对位置相干性的影响。发现腔场的初始态不同,原子间相对位置的退相干情况有所不同。当腔场初始态为热态或Fock态时,原子间相对位置的相干性会周期性的衰减和回复,而当腔场初始态为压缩态时,原子间相对位置会出现部分退相干,且退相干程度与原子间相对位置的大小成余弦变化关系。     

利用两能级原子与腔场相互作用实现纠缠压缩态的纠缠浓缩

根据大失谐条件下原子-腔场相互作用的特点,讨论了一个制备纠缠压缩态的方法,提出了一个利用两能级原子与腔场相互作用实现纠缠压缩态纠缠浓缩的方案。在这个方案中,两束具有相同振幅但有着 相位差的压缩光 和 构成的纠缠态光场被用来作为量子信道。通过利用两能级原子与腔场的相互作用以及两模正交态测量实现了这个纠缠浓缩的过程。结果表明：对于纠缠压缩态,无论其初始的纠缠是多么微弱,利用这种方法总有一定的几率可以从部分纠缠态中提取出最大纠缠态。     

四原子Greenberger-Horne-Zeilinger态的制备

提出了一种制备四原子Greenberger-Horne-Zeilinger 态的方案,它是基于原子-腔场相互作用,首先两个分离的腔初始时处于真空态,通过双光子转移把两个腔制备成缠结态。随后,与腔场发生共振相互作用的4 个等同的原子被分别送入两个腔,通过相互作用后,4 个原子处于GHZ态,而两个腔仍然处于真空态。     

A Theoretical Scheme for Entanglement Transfer under Intensity-Dependent Couplings

We consider a theoretical scheme for entanglement transfer between a two-mode squeezed vacuum field and two initially separable atoms through intensity-dependent couplings. We find that the entanglement transfer between the field and the atoms has an exact period for any given squeezing. We also find that the maximum achievable entanglement of the atomic subsystem is a simple increasing function of r.For sufficiently large squeezing parameter r, it is possible for the atoms to be entangled into a Bell state at half the periodic time points.     

耦合双原子Jaynes-Cummings模型的腔场谱H

研究了处于激发态的两原子与高Q腔场相互作用单光子过程的腔场谱,给出了初始光场为光子数态、相干态、压缩真空态时的腔场谱数值计算结果,分析了原子间偶极-偶极相互作用强度gα对腔场谱结构的影响.发现真空场Rabi峰,当gα较弱时为4峰,gα较强时为3峰结构;弱场数态(n＞0)时为5峰,强场时为3峰结构.相干态和压缩真空态时,谱结构与光子数分布有关,一般为复杂的多峰结构.结果表明,gα对峰位峰高都有影响,破坏了谱结构的对称性,但这种影响只在真空场和弱场时才较明显.     

Complete entanglement transfer between light and qubits

Using the two-mode two-photon Jaynes-Cummings model, entanglement transfer between atoms and field is studied. It is found that when the field is in state constructed from the two-mode photon number states |00〉,|11〉 or the two-mode squeezed vacuum states, full entanglement exchange can be attained no matter the atoms are initially in pure or mixed states. These investigations show that CV entangled states can act as perfectly as the entangled number states in entangling initially separable atoms. The two-mode two-photon atom-field interaction also provides a simple way for the quantum teleportation of atomic or field states.     

单模辐射场与耦合双原子相互作用系统中场熵的压缩特性

研究了单模辐射场与耦合双原子相互作用系统中场熵的压缩特性,讨论了系统初始状态及原子间偶极相互作用对场熵压缩特性的影响.数值计算结果表明,当系统初始时刻处于合适的相干叠加态时,场熵呈现出周期性压缩现象,其压缩深度和压缩时间与原子间偶极相互作用强度有关. 关键词： 单模辐射场 耦合双原子 光场熵压缩     

Entanglement Dynamics of Two Atoms in the Squeezed Vacuum and the Coherent Fields

We investigate the entanglement dynamics of two atoms in a double damping Jaynes-Cummings model. The two atoms are initially in the Bell states and each is in a squeezed vacuum cavity field or coherent cavity field. Compared with the case in coherent field, the atomic entanglement in the squeezed vacuum field is stronger under the same conditions. The results show that we can adopt appropriate parameters such as mean photon number, detuning, the atomic spontaneous decay and the cavity decay, to realize better control of atomic entanglement in quantum information processing. What’s worth mentioning is that proper choosing of the last two parameters enables us to decrease disentanglement period and postpone the moment when the entanglement disappears. Finally, the atomic entanglement in double damping and non-identical Jaynes-Cummings model is obtained

     

Ξ型三能级原子玻色-爱因斯坦凝聚体对光场压缩性质的影响

利用格子液体方法对Ξ型三能级原子玻色-爱因斯坦凝聚体与单模压缩相干态光场相互作用系统的哈密顿量进行了改进, 并且研究了Ξ 型三能级原子单模光场系统中光场压缩性质.结果表明: 光场两正交分量交替呈现周期性压缩, 其最大压缩深度由光场与原子间的相互作用强度和光场初始压缩因子决定, 而压缩时间与光场的圆频率有关. 关键词： 玻色-爱因斯坦凝聚 Ξ型三能级原子 压缩相干态 单模压缩态光场     

Entangling Two Multi-atomic Clusters Through a Cavity Field

Two atomic clusters, which have NA and Ns two-level atoms, respectively, are placed in a cavity but separated spatially. There is no direct interaction between the atoms. All the atoms interact with a single-mode of the cavity field. Quantum entanglement between the two atomic clusters is investigated for various initial states of the two atomic clusters and the field. When the cavity field is initially in a Fock state, we find that the time evolution of entanglement quasi-periodically oscillates regardless of the initial states of atoms. The oscillation period increases as the initial photon number increases. When all the atoms in both of the atomic clusters are initially in the excited state, we show that there is no entanglement between the atomic clusters with NA = NB = 1 regardless the initial state of the cavity field. However, when either NA or NB is larger than one, we find that the entanglement always exists even for a strong thermal field. In cases with different initial states of the atomic clusters, we notice that the entanglement becomes stronger as number of the atoms increases. When all the atoms in both of the clusters in the ground state, we also find that the entanglement can be enhanced even by a thermal field. We also notice that a single qubit can be entangled with multi-atoms which are initially in the ground state by the cavity field initially being in vacuum, thermal, coherent, and squeezed states.     

Nonlocal Correlations of Moving Three-level Atoms in Photon-added Squeezed Thermal States

We investigate nonlocal correlations between a three-level atom and the optical field initially being in the photon-added squeezed thermal state. We examine the effect of the squeezing parameter and the number of added photons to the squeezed thermal field on the entanglement during the time evolution. We show that the entanglement can be enhanced by increasing the number of added photons and the squeezing parameter for moving and nonmoving three-level atoms. We present a useful way to generate and restrain a large amount of entanglement by increasing the number of added photons when the atomic motion is described by the atomic velocity.     

A theory of two-photon light generation involving inversionless two-level atoms

We propose a theory that makes it possible to examine both laser and micromaser two-photon light generation. The theory is based on the Lamb-Scully model, in which two-level atoms have initial coherence. Such an initial state allows for light generation involving atoms without inversion or even atoms with negative population inversion in the transition. We analyze the conditions needed for the emergence of squeezed states of the light field. We also show that the photon statistics in lasing is always classical but that there appears a state of the field squeezed in the phase with maximum photodetection shot-noise suppression. For a micromaser we find a regime where sub-Poisson light with a shot-noise suppression level of 60% is realized in an inversionless transition. In another regime, a squeezed state that produces 75% suppression of noise can be generated. Zh. éksp. Teor. Fiz. 115, 1605–1618 (May 1999)