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Interference Effects in a Photonic Crystal Cavity

机译:光子晶体腔中的干涉效应

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We investigate quantum interference and classical interference effects when a three-level system interacts with both a cavity field mode and an external driving field mode, within the confines of a photonic crystal material. In free-space, we found that under certain circumstances the cavity field evolves to be equal in magnitude to, but 180° out-of-phase with the external pump field when the pump field frequency equals the cavity frequency. The better the cavity, the quicker this build-up occurs. When the cavity field reaches this out-of-phase condition, the resonance fluorescence from the atom in the cavity goes to zero. This is a purely classical interference effect between the two out-of-phase fields, with the resonance fluorescence going to zero at the same time as the two excited state populations go to zero. This is quite different from the quantum interference that occurs under the right circumstances, when the state populations are coherently driven into a linear combination that is decoupled from any applied field - and population is trapped in the excited states, thus allowing for a population inversion and an amplification of incoming optical signals. In this paper, we investigate the additional effects due to the presence of the altered photon density of states in a photonic crystal.
机译:当三能级系统在光子晶体材料的范围内与腔场模式和外部驱动场模式相互作用时,我们研究了量子干涉和经典干涉效应。在自由空间中,我们发现在某些情况下,当泵浦场频率等于腔室频率时,腔场在大小上会与外部泵浦场相等,但与外部泵浦场异相180°。空腔越好,这种积聚就越快。当腔场达到此异相条件时,来自腔中原子的共振荧光将变为零。这是两个异相场之间的纯经典干扰效应,共振荧光在两个激发态总体趋于零的同时变为零。这与在适当情况下发生的量子干扰完全不同,在正确的情况下,当状态总体被相干地驱动为与任何应用场分离的线性组合时,总体被捕获在激发态中,从而允许总体反转和输入光信号的放大。在本文中,我们研究了由于光子晶体中改变的光子态密度而引起的附加效应。

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