四极子微腔的光场分布  被引量:1

Optical-Field Distribution of Quadrupolar-Shaped Microcavity

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作  者:李赞佳[1] 吴根柱[1] 凤兰[1] 霍海燕[1] 

机构地区:[1]内蒙古大学物理系,呼和浩特010021

出  处:《光学学报》2007年第5期903-906,共4页Acta Optica Sinica

基  金:国家自然科学基金(60366001)资助项目

摘  要:应用电磁场理论和介质中的麦克斯韦方程组,推导了任意截面微腔的TM模光场分布。并以四极子状微腔截面为例,推导了含有传播常数的本征方程。用Mathematica软件模拟出具有不同变形因子的基模(m=1)和高阶模的光场分布图,得出基模在Φ=45°,135°,225°,315°四个方向光辐射最强,具有“蝴蝶结模式”特征,并且当变形因子值取ε’为0.1~0.15时,该效应表现得更明显;而高阶模(m≥2)时微腔中没有这种光的定向输出现象,在任何变形因子情况下也不能形成稳定的“蝴蝶结模式”,为四极子微腔激光器的设计和制作提供了一定的理论依据。Using the theory of electromagnetic field and Maxwell equations in medium, we derive the TM mode optical field distribution of resonators with arbitrary cross section. Moreover, taking quadrupolar-shaped microcavity as example, it deduces the eigenvalue equation which contains the propagation constant. Using the software Mathematica, it stimulates the optical field distribution of fundamental mode (m=1) and high-order mode with the different deformation factors, and it is found that the fundamental mode gets the maximum of light emission at Φ=45°, 135°, 225°, 315°, it has the feature of "bow-tie" mode. Furthermore, when the deformation factor is 0.1~0.15, the effect is more obviously; however there is not the phenomenon of drawing out the light directionally in the microcavity when m ≥2, and it does not form the stable "bow-tie" mode when the deformation factor gets any values. It provides a certain theoretical base for designing and making the quadrupolar-shaped microcavity lasers.

关 键 词:光计算 四极子 微腔 光场分布 变形因子 

分 类 号:TN25[电子电信—物理电子学]

 

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