摘要
利用纠缠态表象下的维格纳(Wigner)算符,构造了双模激发压缩真空态的维格纳函数,并根据该函数在相空间ρ-γ中随参量m,n和r的变化关系,讨论了双模激发压缩真空态的量子干涉特性和压缩效应。结果表明,对于参量m,n不同的取值,双模激发压缩真空态的量子干涉效应的强弱不同;而对于不同的压缩参量r,双模激发压缩真空态呈现出不同程度的压缩效应。最后,根据双模激发压缩真空态的维格纳函数的边缘分布,阐明了此维格纳函数的物理意义。
Using the Wigner operator in the entangled-state representation we construct the Wigner functions of the two-mode excited squeezed vacuum states (TESVS). In term of the variations of the Wigner functions with respect to the parameters m, n and r in the ρ-γ phase space, the quantum interference properties and squeezing effects of the TESVS are discussed. The results show that, for different values of m and n, the TESVS have different quantum interference effects, however for different squeezing parameters r the TESVS exhibit different squeezing effects. Furthermore, the physical meaning of the Wigner functions is identified according to the marginal distributions of the Wigner functions for the TESVS.
出处
《光学学报》
EI
CAS
CSCD
北大核心
2007年第9期1700-1705,共6页
Acta Optica Sinica
基金
国家自然科学基金(10574060)
山东省自然科学基金(Y2004A09)资助的课题
关键词
量子光学
双模激发压缩真空态
纠缠态表象
维格纳函数
边缘分布函数
quantum optics
two-mode excited squeezed vacuum state
entangled-state representation
Wigner function
marginal distribution function