利用充分本征值问题建立半导体微腔激光的数学模型

A. Nosich
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引用次数: 0

摘要

从分析可以得出,无阈值激光器并不比永动机更现实。事实上,当人们注意到无限光子晶体显示出没有电磁波可以传播的频率带隙时,无阈值激光的思想就出现了。因此,微晶体或缺陷腔激光在光子晶体介质中可能具有零阈值。然而,没有晶体是无限的,因此阈值只能很小。实际上,零阈值完全等同于零输出光。因此,无限光子晶体中激光的分析要么是错误的,如果用近似的或粗糙的数值方法,如FDTD,要么是没有意义的,如果用精确的方法,正确地解释辐射条件。相反,人们必须简单地用一个有限尺寸的光子晶体包裹一个激光谐振器来制定LEP,并研究阈值的降低作为基本单元尺寸、拓扑、填充和数量的函数。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Mathematical modeling of lasing in semiconductor microcavities by means of adequate eigenvalue problems
From the analysis it follows that a thresholdless laser is not more realistic than a perpetual motion machine. In facts thresholdless lasing idea had appeared when it was noticed that infinite photonic crystals display frequency bandgaps, in which no electromagnetic wave can propagate. Therefore, it was suggested that a microcrystal or defect-cavity laser in a photonic crystal host medium might have zero threshold. However, no crystal is infinite, therefore the thresholds can be only made small. In fact, zero threshold is completely equivalent to zero output light. Therefore it appears that analyses of lasing in infinite photonic crystals are either erroneous, if done approximately or with coarse numerical methods like FDTD, or has no sense at all, if done with accurate methods, which correctly account for the radiation conditions. Instead, one must simply formulate the LEP with a finite-size photonic-crystal encasing a laser resonator and study the reduction of the thresholds as a function of elementary cell size, topology, filling, and number.
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