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态|Ψ(3)q中广义电场分量的不等幂次Nj次方Y压缩
引用本文:万慧军,杨志勇,胡晓云,余晓光,周美娟,李春.态|Ψ(3)q中广义电场分量的不等幂次Nj次方Y压缩[J].光子学报,2003,32(4):489-493.
作者姓名:万慧军  杨志勇  胡晓云  余晓光  周美娟  李春
作者单位:1. 西北大学光子学与光子技术研究所,西北大学光电子技术省级重点开放实验室,西安,710069;井冈山师范学院物理系,江西,吉安,343009
2. 西北大学光子学与光子技术研究所,西北大学光电子技术省级重点开放实验室,西安,710069;西安电子科技大学技术物理学院,西安,710071
3. 西北大学物理学系,西安,710069
4. 井冈山师范学院物理系,江西,吉安,343009
5. 西北大学光子学与光子技术研究所,西北大学光电子技术省级重点开放实验室,西安,710069井冈山师范学院物理系,江西,吉安,343009
基金项目:陕西省自然科学基金(批准号:2001SL04;2000SL10)、陕西省教育厅专项科研基金(批准号:99JK091;00JK115)和西北大学科学基金(批准号:99NW38)资助项目
摘    要:利用多模压缩态理论,研究了由多模复共轭虚相干态|{iZj*}〉q、多模复共轭虚相干态的相反态|{-iZj*}〉q和多模复共轭相干态|{Zj*}〉q的线性叠加所组成的新型三态叠加多模叠加态光场|Ψ(3)q中广义电场分量的偶数次不等幂次Nj次方Y压缩特性.结果发现:在各模的压缩次数Nj=2pjpj=2mj+1(mj=0,1,2,3,…,…)和Nj′=2pj′且pj′=2mj′+1(mj′=0,1,2,3,…,…)的条件下,当各模的初始相位φjφj′、态间的初始相位差(θ13)与(θ23),以及各单模相干态光场总的平均光子数之和qj=1R2j等分别满足一定的取值条件时,态|Ψ(3)q的广义电场分量(即第二正交相位分量)总可呈现出周期性变化的、偶数次的广义非线性不等幂次Nj次方Y压缩效应.

关 键 词:三态叠加  多模叠加态光场  广义电场分量  不等幂次Nj次方Y压缩  多模压缩态
收稿时间:2002/6/3
修稿时间:2002年6月3日

Even-number-power Generalized Nonlinear Unequal-Power Nj-th Power Y-Squeezing of Generalized Electric Field Component in the State |Ψ(3)〉q
Wan Huijun,Yang Zhiyong,Hu Xiaoyun,Yu Xiaoguang,Zhou Meijuan,Li Chun.Even-number-power Generalized Nonlinear Unequal-Power Nj-th Power Y-Squeezing of Generalized Electric Field Component in the State |Ψ(3)〉q[J].Acta Photonica Sinica,2003,32(4):489-493.
Authors:Wan Huijun  Yang Zhiyong  Hu Xiaoyun  Yu Xiaoguang  Zhou Meijuan  Li Chun
Institution:1. Institute of Photonics &; Photon-Technology, and Provincial Key Laboratory of Photoelectronic Technology, Northwest University, Xi′an, 710069, P.R.China;
2. Department of Physics, Jinggangshan Normal College, Ji′an, Jiangxi, 343009, P.R.China;
3. School of Technology and Physics, Xidian University, Xi′an 710071, P.R.China;
4. Department of Physics, Northwest University, Xi′an, 710069, P.R.China
Abstract:It is studied systematically that even-number-power generalized nonlinear unequal-power Nj-th power Y-squeezing properties of generalized electric field component in a new type of three state superposition multimode superposition state light field |Ψ(3)> q which is made of the multimode complex conjugation imaginary coherent state |{iZj*}〉q, the contrary state |{iZj*}〉q of multimode complex conjugation imaginary coherent state |{iZj*}〉q, and the multimode complex coherent state |{iZj*}〉q, by utilizing the multimode squeezed state theory established recently. It is found that if the squeezed-power-number of each mode in the state |Ψ(3)q both Nj=2pj, pj=2mj+1(m′(here j=0,1,2,3,…,…) and pj′=2mj′+1(m′(here j′=0,1,2,3,…,…), while some certain conditions are satisfied respectively by the initial phase φj and φj′ of each mode in the state |Ψ(3)q, by the initial phase difference(θ13)and(θ23)between any two components in the state |Ψ(3)q, and by the sum of mean photon-numbers of all the single-mode coherent state light field, the generalized electric field component(or the second perpendicular phase component)in the state |Ψ(3)q can always display the effects of even-number-power generalized nonlinear unequal-power Nj-th power Y-squeezing which changes periodically.
Keywords:Three state superpositions  Multimode superposition state light field  Generalized electric field component  Unequal-power N  j-th power Y-squeezing  Multimold squeezed state
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