耗散环境下原子-库场相互作用系统中原子的偶极压缩特性  

Dipole squeezing of atomic systems in dissipative environment

作　　者：潘长宁[1] 赵学辉[1] 杨迪武[1] 方卯发[2] 

机构地区：[1]湖南工业大学理学院,株洲412008 [2]湖南师范大学物理与信息科学学院,长沙410081

出　　处：《物理学报》2010年第10期6814-6818,共5页Acta Physica Sinica

基　　金：国家自然科学基金(批准号:50874041);湖南省教育厅自然科学基金(批准号:09C314);湖南省自然科学基金(08JJ5036)资助的课题~~

摘　　要：运用全量子理论并结合数值计算方法,研究了处于真空库和热库中原子系统的偶极压缩特性,讨论了原子的初态以及热库的平均光子数对原子偶极压缩特性的影响.研究表明:真空库中,初始处于基态和激发态的叠加态原子,当激发态的粒子布居概率少于基态时,原子的偶极压缩无限接近于零而永远不消失;反之,原子的偶极压缩将在有限的时间内消失;热库中,不管原子初始处于什么态,其偶极压缩都在有限的时间内消失,并且随着热库的平均光子数的增大而消失得越快。The atomic squeezing effect in the dissipative environment is investigated by means of the quantum theory of dampingdensity operator approach and numerical calculations.The effects on the atomic dipole squeezing effect produced by the atomic initial state and mean photon number of the thermal reservoir are discussed.The results show that the atomic dipole squeezing declines asymptotically to zero,and doesn＇t disappear in finite time if the population rate in the excited state is higher than the ground state in the atomic initial state in the vacuum reservoir.However,the squeezing effect always disappears in the thermal reservoir,irrespective of the atomic initial state.With increase of mean photon of the thermal reservoir,the squeezing effect disappears faster.

关 键 词：耗散环境 真空库 热库 偶极压缩 

分 类 号：O431.2[机械工程—光学工程]