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Interference Effects in a Photonic Crystal Cavity

机译:光子晶体腔中的干扰效应

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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° outof-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:当三级系统与腔场模式和外部驱动场模式相互作用时,在光子晶体材料的范围内,研究量子干扰和经典干扰效应。在自由空间中,我们发现在某些情况下,当泵场频率等于空腔频率时,腔场的幅度为相等,但是与外部泵场的外部相位相等。腔腔越好,这种积累的速度越快。当腔场达到这种超相位的条件时,来自腔中的原子的共振荧光变为零。这是两个超阶段字段之间的纯粹经典干扰效果,同时谐振荧光与两个激动的状态群相当于零。这与在合适的环境下发生的量子干扰是完全不同的,当状态群体被连贯地被驱动到从任何应用的场地解耦的线性组合 - 并且群体被困在激发态中,从而允许人口反转和引入光信号的放大。在本文中,我们研究了由于光子晶体中的状态改变的光子密度的存在而导致的附加效果。

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