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Ultralow Raman lasing threshold and enhanced gain of whispering gallery modes in silica microspheres

机译:二氧化硅微球中超低拉曼激光阈值和耳语回波模式增强增益

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摘要

Remarkable demonstrations of a cavity-induced giant reduction of the Raman lasing threshold in silicanmicrospheres have been reported in Spillane et al. [Nature (London) 415, 621 (2002)], yet a complete quantumnelectrodynamics (QED) treatment of this process including the rigorous expressions for the electromagneticnmodes of the sphere is lacking. In this paper, we employ a cavity QED approach to describe Raman lasingnin microscopic spherical dielectric resonators with third-order nonlinearity to derive explicit expressions fornthe Raman gain and lasing threshold in terms of mode-overlapping coefficients determined from full analyticnexpressions of the electromagnetic eigenmodes of a dielectric sphere. We present dependencies of the Ramannlasing threshold on the the order n of overlapping whispering gallery modes for microspheres with diameternin the range 20–35 μm, demonstrating ultralow thresholds of between 70 and 90 μW, consistent with recentnexperimental results. We explain the reduction of the lasing threshold as due to an increase in the overlappingncoefficients as the mode order is increased toward the regime where the modal energy is mostly confined to thensurface region of the resonator. The presented theory can be easily generalized to any microcavity of regularnmorphology and for any combination of interacting whispering gallery modes.
机译:Spillane等报道了在硅微球中腔诱导的拉曼激射阈值的巨大降低的显着证明。 [Nature(London)415,621(2002)],但是缺少对该过程的完整量子电动力学(QED)处理,包括对球体电磁模的严格表达。在本文中,我们采用腔QED方法来描述具有三阶非线性的拉曼lasingnin微观球形介电谐振器,以根据由电子的本征模的全解析表达式确定的模式重叠系数来得出拉曼增益和激射阈值的明确表达式。介电球。对于直径在20-35μm范围内的微球,我们提出了Ramannlasing阈值对重叠耳语画廊模式阶数n的依赖性,表明超低阈值介于70和90μW之间,与最近的实验结果一致。我们解释了激射阈值的减小,这是由于随着模态阶数朝着模态能量主要限于谐振器的表面区域的状态而增加,随着重叠系数的增加。提出的理论可以很容易地推广到任何正态形态的微腔以及相互作用的耳语画廊模式的任何组合。

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  • 来源
    《PHYSICAL REVIEW A》 |2012年第1期|1-7|共7页
  • 作者单位

    Center for Superfunctional Materials Department of Chemistry and Department of Physics Pohang University of Science and TechnologyPohang 790-784 Korea;

    Center for Superfunctional Materials Department of Chemistry and Department of Physics Pohang University of Science and TechnologyPohang 790-784 Korea;

    Center for Superfunctional Materials Department of Chemistry and Department of Physics Pohang University of Science and TechnologyPohang 790-784 Korea;

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