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第Ⅵ类两态叠加多模叠加态光场的广义非线性等阶N次方H压缩
引用本文:侯瑶,田来科,董庆彦,王菊霞,杨志勇,孙秀泉.第Ⅵ类两态叠加多模叠加态光场的广义非线性等阶N次方H压缩[J].光子学报,2001,30(12):1442-1448.
作者姓名:侯瑶  田来科  董庆彦  王菊霞  杨志勇  孙秀泉
作者单位:1. 西北大学物理学系,西安,710069
2. 渭南师范学院量子光学与光子学研究室,渭南,714000
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西北大学现代物理研究所,西安,710069
基金项目:陕西省自然科学基金(批准号:2000SLl0)、陕西省教育厅专项科研基金(批准号:99JK091)和西北大学科学基金(批准号:99NW38)资助项目
摘    要:本文根据量子力学中的线性叠加原理,构造了由多模相干态|{Zj}〉q与多模虚相干态|{iZj}〉q这两者的线性叠加所组成的第类两态叠加多模叠加态光场|φ6(2)q.利用多模压缩态理论,研究了态|φ6(2)q的广义非线性等阶N次方H压缩特性.结果发现:1)在腔模总数q与压缩阶数N这两者之积取偶数亦即qN=2p的条件下,如果p=2l(l=1,2,3,…,…),则无论各模的初始相位和∑j=1qφj、态间的初始相位差(θpq(R)pq(I))以及各单模相干态光场的平均光子数之和∑j=1qRj2等如何变化,态|φ6(2)q总是恒处于等阶N-H最小测不准态.2)在qN=2p的条件下,如果p=2l+1(l=0,1,2,3,…,…),则当∑j=1qφj、(θpq(R)q(I))、∑j=1qRj2、(θpq(R)q(I))-∑j=1qRj2]等分别满足一定的量子条件(或者在一些特定的闭区间内连续取值)时,态|φ6(2)q总可呈现出周期性变化的等阶N次方H压缩效应.

关 键 词:两态叠加  多模叠加态光场  等阶N-H最小测不准态  等阶N次方H压缩效应
收稿时间:2001-06-20
修稿时间:2001年6月20日

THE PROPERTIES OF GENERALIZED NONLINEAR EQUAL-ORDER N-TH POWER H-SQUEEZING IN THE SIXTH KIND OF MULTIMODE SUPERPOSITION STATE LIGHT FIELD WITH THE SUPERPOSITIONSOF A MULTIMODE COHERENT STATE AND A MULTIMODE IMAGINARY COHERENT STATE
Hou Yao,Tian Laike,Dong Qingyan,Wang Juxia,Yang Zhiyong,Sun Xiuquan.THE PROPERTIES OF GENERALIZED NONLINEAR EQUAL-ORDER N-TH POWER H-SQUEEZING IN THE SIXTH KIND OF MULTIMODE SUPERPOSITION STATE LIGHT FIELD WITH THE SUPERPOSITIONSOF A MULTIMODE COHERENT STATE AND A MULTIMODE IMAGINARY COHERENT STATE[J].Acta Photonica Sinica,2001,30(12):1442-1448.
Authors:Hou Yao  Tian Laike  Dong Qingyan  Wang Juxia  Yang Zhiyong  Sun Xiuquan
Institution:1. Department of Physics, Northwest University, Xi’an 710069;2. Research Section of Quantum Optics & Photonics, Wei’nan Normal College, Wei’nan 714000;3. Institute of Photonics & Photon-Technology, and Provincial Key Laboatory of Photoelectronic Technology, Northwest University, Xi’an 710069;4. Institute of Modern Physics, Northwest University, Xi’an 710069
Abstract:According to the linear superposition principle of quantum mechanics, in this paper, the sixth kind of multimode superposition state light field |φ6(2)q which is composed of the linear superposition of multimode coherent state |{Zj}〉q and multimode imaginary coherent state |{iZj}〉q is constructed.By utilizing the theory of multimode squeezed states established by Yang Zhiyong and Hou Xun and published in Acta Photonica Sinica from the April of 1998 to the May of 1999,the properties of generalized nonlinear equal-order WTBXN-th power H-squeezing of the state |φ6(2)q mentioned above is studied firstly in detail.It is found that 1)under the condition of the products of total cavity-mode-number and squeezing-order-mumber or qN=2p and p=2l (here,l=1,2,3,...,...,),the state |φ6(2)q is always stayed in the equal-order (or N=4l/q) N-H minimum uncertainty state,whether the initial phase sum ∑j=1qφj of all modes,the initial phase difference (θpq(R)pq(I)) between the two compenents |{Zj}〉q and |{iZj}〉q mentioned,and the sum ∑j=1qRj2 of mean photon number of each single-male coherent state light field in the state |φ6(2)q,WTBZand the phase difference JB(θpq(R)pq(I)-∑j=1qRj2] change or not.
Keywords:Superpositions of macroscopically distinct two quantum states  Multimode superposition state light field  Equal-order N-H minimum uncertainty state  Equal-order N-th power H-sqreezing effect  
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