摘要
研究了振幅相干态的Pegg-Barnett量子相位密度分布,结果发现,1)影响振幅相干态的量子相密度分布P(θ,m)的物理条件有:真空态|O〉与是相干态|α〉相叠加的角度φ,平均光子数和量子相位角θ与相干态移动相位角γ的相对值θ-γ。2)量子相密度分布相对φ、θ-γ作周期变化;它随平均光子数的增大而增大;一定条件下φ、θ-γ影响振幅相干态的量子相密度分布的极值。
Pegg-Barnett Quantum phase density distribution properties of amplitude coherent states are studied. It is find that: 1. the Quantum phase density distribution of amplitude coherent states p(θ,m) is influenced by superposition angle φ which is the vacuum state |o〉 superposed by coherent state|α〉, average photon number and θ-γ that is the quantum phase θ minus displace angle of coherent state γ. 2. the quantum phase density distribution changes with φ and θ-γ periodically; it becomes large with increase of average photon numbers. Under certain conditions, extremums of quantum phase density distribution are restricted by φ and θ-γ.
出处
《商洛学院学报》
2008年第5期18-21,共4页
Journal of Shangluo University
基金
陕西省教育厅专项科研基金资助项目(03JK212
04JK125)
关键词
量子光学
振幅相干态
量子相位密度
quantum optics
amplitude coherent state
quantum phase density distribution