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机构地区:[1]宁夏师范学院物理与信息技术学院,宁夏固原756000 [2]渭南师范学院物理与电子工程系,陕西渭南714000
出 处:《科技导报》2010年第16期74-76,共3页Science & Technology Review
基 金:陕西省教育厅专项科研基金(09JK431);渭南师范学院科研基金项目(09YKS006,09YKZ021)
摘 要:根据量子力学的线性叠加原理,构造了由多模复共轭相干态的相反态{-Zj^(a)*}〉q与多模虚共轭相干态的相反态{-iZj^(b)*}〉q,两者线性叠加组成强度不等的非对称两态叠加多模叠加态光场|ψII^(ab)〉q。利用多模压缩态理论,对态|ψII^(ab)〉q的广义非线性高次压缩性质进行了详细分析。结果发现,若构成态|ψ^II(ab)〉q的两个截然不同的量子光场态{-Zj^(a)*}〉q和态{-iZj^(b)*}〉q中,各对应模的强度(或平均光子数)满足qΣj=1Rj(a)N=qΣj=1R(b)Nj或q∏j=1R(a)Nj=q∏j=1Rj(b)N,并满足一定条件时,无论腔膜总数q、态间初始相位差(θnq(aR)-θnq(bI)),以及两态叠加的概幅rnq(aR)和rnq(bI)等如何变化,态ψII(ab)〉q总可以恒处于等幂次N-Y最小测不准态或等幂次N-H最小测不准态,成为一种新的相干态。In this paper, according to the linear superposition principle in quantum mechanics, non-symmetry state superimposition state light fields ψII(ab )〉q of different intensities are constructed with both the multi-mode complex conjugation coherent state of contrary state {-Z(ja*)}〉q and the multi-mode imaginary conjugation coherent state of contrary state {-iZ(jb*)}〉q, by utilizing the theory of multimode squeezed states, and the properties of the multi-mode superimposition state of differ-intensities of nonsymmetrical superimpositions state with distinguishable two quantum states are studied. It is found that when qΣj=1 R(ja*)N= qΣj=1R(jb*)Nor q∏j=1R(ja)N= q∏j=1R(jb*)N,whilethe quantization conditions are satisfied by the constructed state ψII(ab)〉q with distinguishable two quantum states {-Z(ja*)}〉q and {-iZ(jb*)}〉q of the intensity of the corresponding mode (that is so-called average photon number), no matter how to change the cavity mode and the initial phases of the whole mode, the difference of the initial phases of states (θnq(aR )-θnq(bI)) and the probability amplitude superposition of two states rnq(aR)(or rnq(bI )), the light field state of the superimposition state ψII(ab)〉q is always in the equal-order N-Y minimum uncertainty state and the equal-order N-H minimum uncertainty state.
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