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第Ⅰ类多模叠加态|ψ1(3)q中广义磁场的高次和压缩
引用本文:杨志勇,曹大刚,万慧军,赖振讲,雷小丽,胡艳芳.第Ⅰ类多模叠加态|ψ1(3)q中广义磁场的高次和压缩[J].光子学报,2002,31(9):1041-1046.
作者姓名:杨志勇  曹大刚  万慧军  赖振讲  雷小丽  胡艳芳
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;西北大学现代物理研究所,西安,710069
2. 西北大学学报编辑部,西安,710069
3. 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学系,江西井冈山,343009
4. 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;河南师范大学物理学系,河南新乡,453002
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
基金项目:陕西省自然科学基金(批准号:2001SL10)、陕西省教育厅专项科研基金(批准号:99JK091;00JK115)和西北大学基金(批准号:99NW38)资助项目.
摘    要:构造了由多模相干态|{Zj} > q、多模真空态|{Oj} >q和多模相干态的相反态|{-Zj} > q三者的线性叠加所组成的第Ⅰ类三态叠加多模叠加态光场|ψ1(3) > q,利用多模压缩态理论,研究了态|ψ1(3) > q中广义磁场分量的等幂次高次和压缩效应.结果发现:态|ψ1(3) > q是一种典型的三态叠加多模非经典光场;当各模的初始相位和  order= 满足一定的取值条件、并且态|ψ1(3)q中任意两态的态间初始相位差(θpq(R)0q(0))、(θnq(R)0q(0))和(θpq(R)nq(R))等分别在各自的闭区间内连续变化时,则态|ψ1(3) > q的广义磁场分量(即第一正交相位分量)总可分别呈现出周期性变化的、等幂次的奇数模-偶数次、偶数模-奇数次、偶数模-偶数次或者奇数模-奇数次的高次和压缩效应.

关 键 词:三态叠加  多模非经典光场  广义磁场  等幂次高次和压缩
收稿时间:2002/1/11
修稿时间:2002年1月11日

THE EQUAL-POWER HIGHER-POWER SUM SQUEEZING OF GENERALIZED MAGNETIC FIELD COMPONENT IN THE FIRST KIND OF THREE STATE SUPERPOSITION MULTIMODE SUPERPOSITION STATE LIGHT
Yang Zhiyong ,Cao Dagang ,Wan Huijun ,Lai Zhenjiang , Lei Xiaoli ,Hu Yanfang Institute of Photonics & Photon Technology,and Provincial Key Laboratory of Photoelectronic Technology,Northwest University,Xi'an.THE EQUAL-POWER HIGHER-POWER SUM SQUEEZING OF GENERALIZED MAGNETIC FIELD COMPONENT IN THE FIRST KIND OF THREE STATE SUPERPOSITION MULTIMODE SUPERPOSITION STATE LIGHT[J].Acta Photonica Sinica,2002,31(9):1041-1046.
Authors:Yang Zhiyong    Cao Dagang  Wan Huijun    Lai Zhenjiang  Lei Xiaoli  Hu Yanfang Institute of Photonics & Photon Technology  and Provincial Key Laboratory of Photoelectronic Technology  Northwest University  Xi'an
Institution:Yang Zhiyong 1,2,Cao Dagang 3,Wan Huijun 1,4,Lai Zhenjiang 1,5 Lei Xiaoli 1,Hu Yanfang 1 1 Institute of Photonics & Photon Technology,and Provincial Key Laboratory of Photoelectronic Technology,Northwest University,Xi'an 710
Abstract:The first kind of the three state superposition multimode superposition light field |ψ1(3) > q is constructed that is made of multimode coherent state light field |{Zj} > q 、multimode vaccum state light field |{Oj} > q and contrary state |{Zj} > q of multimode coherent state and that is based upon the linear superposition principle of quantum state in quantum mechanics in this paper. Then the multimode squeezed state theory is utilized to study the properties of equal-power higher power sum-squeezing of generalized magnetic field component in the state |ψ1(3) > q in detail. It is found that the state |ψ1(3) > q is a new type of three state superposition multimode nonclassical light field, while some certain conditions are satisfied bythe initial phase sum qj=1φj of each mode in the state |ψ1(3) > q, and while the initial phase difference(θpq(R)0q(0))、(θnq(R)0q(0))and(θpq(R)nq(R))between any two states in the state |ψ1(3) > q change continuously within their own fixed and closed regions respectively, the generalized magnetic field component(or the first perpendicular phase component)of the state |ψ1(3) > q can always display the generalized nonlinear equal-power odd number mode with even-number-power, even number mode with odd number power, even number mode with even-number-power, and odd number mode with odd number power higher power sum-squeezing, respectively, which changes periodically.
Keywords:Three state superpositions  Multimode nonclassical light field  Generalized magnetic field  Equal  power higher  power sum squeezing
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