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用时域有限差分法研究了一维光子晶体多量子阱中的谱线分裂现象,揭示了光子隧穿多量子阱时谱线分裂的规律性.研究发现,谱线分裂是阱间相互耦合的结果,其特征不仅取决于势阱的个数,而且与垒区和阱区的几何参量密切相关.计算结果表明,对称多量子阱结构中,光子隧穿p个势阱时,单阱对应的每条透射谱线会分裂为p条,各分裂谱线互不交叠.这样在有限的禁带区域可以成倍增加光子束缚态,使信道密度最大化,光波有效带宽的使用最优化,有望在光通信超密集波分复用和光学精密测量中获得广泛应用.

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