OFS Laboratories, 19 Schoolhouse Road, Somerset, New Jersey 08873, USA.
Opt Lett. 2010 Jul 15;35(14):2385-7. doi: 10.1364/OL.35.002385.
As opposed to the modes in an optical spherical/spheroidal microresonator, the whispering gallery modes in a long cylindrical microresonator are delocalized. Consequently, a circulating light beam that is evanescently coupled into the cylinder and experiences total internal reflection eventually radiates out along the cylinder axis. However, the self-interference of such a beam can produce a resonant mode that is strongly localized along the axial direction. Specifically, the mode characteristic width is (alphabeta)(-1/2), where alpha and beta are the attenuation and propagation constants of the cylinder material. The Q-factor of this mode can be almost as large as the Q-factor of modes in a spheroidal microresonator with the same alpha divided by 2.542.
与光学球型/球壳微谐振器中的模式相反,长圆柱形微谐振器中的 whispering gallery 模式是弥散的。因此,一个在圆柱体内渐逝耦合并经历全内反射的循环光束最终会沿着圆柱轴辐射出去。然而,这种光束的自干涉可以产生一个沿着轴向强烈局域的共振模式。具体来说,该模式的特征宽度为(alphabeta)^(-1/2),其中 alpha 和 beta 是圆柱材料的衰减和传播常数。该模式的 Q 因子几乎可以与具有相同 alpha 的球壳微谐振器中的模式的 Q 因子一样大,除以 2.542。