首页> 外文期刊>Optics Communications: A Journal Devoted to the Rapid Publication of Short Contributions in the Field of Optics and Interaction of Light with Matter >On the quantum phase fluctuations of coherent light in a chain of two anharmonic oscillators coupled through a linear one
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On the quantum phase fluctuations of coherent light in a chain of two anharmonic oscillators coupled through a linear one

机译:关于两个通过线性耦合的非谐振荡器的相干光中相干光的量子相位涨落

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We investigate the quantum phase fluctuations of input coherent light involving two quartic anharmonic oscillators coupled through a linear one. The analytical expressions for various phase fluctuation parameters due to Carruthers and Nieto are expressed as functions of coupling constant, anharmonic constant, initial excitation numbers, and the initial phase of the input coherent field. By using some numerical estimates of the analytical expressions, the effects of anharmonic and coupling constants are clearly indicated. In one of the two anharmonic modes (say mode a(1)), it is found that the presence of coupling causes the reduction of phase fluctuation parameters U-1, and S-1, compared to their counterparts at t=0. In sharp contrast to these results, the increase and the decrease (at least in the axis range of kt) of the phase fluctuation parameters U-1, S-1 and Q(1) compared to their initial value counterpart are attributed by the strong field and hence the nonlinearity. We establish that the signature of anharmonicity (beta not equal 0) is realized only for intense field situations. It corroborates the fact that the nonlinearity of the medium is invoked only if the field strength is quite strong. Interestingly, for significantly strong field situation, the reduction of the phase fluctuation parameters compared to their initial values is exhibited for the harmonic mode. These reductions are attributed partly by the strong field and partly by the coupling between the oscillators. In spite of the modes corresponding to two anharmonic oscillators which are in vacuum, we report the generation of excitation for nonzero coupling constant with beta=0. It may be attributed by the quantum state transfer through the chain of harmonic oscillators. (C) 2016 Elsevier B.V. All rights reserved.
机译:我们研究了涉及通过线性耦合的两个四次非谐振荡器的输入相干光的量子相位波动。由Carruthers和Nieto引起的各种相位波动参数的解析表达式表示为耦合常数,非谐常数,初始激励数和输入相干场的初始相位的函数。通过使用一些解析表达式的数值估计,可以清楚地表明非谐和耦合常数的影响。在两种非谐模式之一(例如模式a(1))中,发现与t = 0时的相变参数相比,耦合的存在导致相位波动参数U-1和S-1减小。与这些结果形成鲜明对比的是,相变参数U-1,S-1和Q(1)相对于其初始值对应物的增大和减小(至少在kt轴范围内)是由于场和非线性。我们确定,仅在强场情况下才能实现非谐性(β不等于0)的签名。这证实了只有在场强相当强的情况下才调用介质的非线性这一事实。有趣的是,对于强磁场情况,对于谐波模式,相位起伏参数与其初始值相比有所降低。这些减少部分归因于强磁场,部分归因于振荡器之间的耦合。尽管与处于真空中的两个非谐振荡器相对应的模式,我们仍报告了β= 0时非零耦合常数的激励产生。这可能归因于通过谐波振荡器链的量子态转移。 (C)2016 Elsevier B.V.保留所有权利。

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