论文标题
两个亚波长介质谐振器中极高的Q因子的工程
Engineering of the extremely high Q factor in two subwavelength dielectric resonators
论文作者
论文摘要
可以通过Rybin {\ It et al} [Phys Phys Phys Phys Phys Phys Phys Phys Physe vyphys notortorthe {莱特牧师。 119,243901(2017)]。与以前的一个参数避免在分离的磁盘中避免过境的情况相比,在两个参数上遍历两个参数和两个磁盘之间的距离,可以增强Q因子几倍。因此,连续的两参数避免过境,可以正如预期的那样在Q因子中产生多重增益。但是,如果对于单个磁盘,其正交谐振模式不会避免穿越,则第二盘的存在会可以消除这种限制,并引起这些模式的避免穿越,与单个磁盘相比,$ q $ factor的范围将$ q $ factor提高了两个订单。反键谐振模式的多极分解表明,如Chen {\ it等} [Laser&PhotonicsReviews 13,1900067(2019)所示的多极模式的较低顺序到较高的多极模式的转换。这些结果可以解释出最大转换处的场构型与在等效球中具有高轨道动量的MIE共振模式接近。对于M = 1,谐振模式泄漏到两种类型的连续图中,该模式大大降低了亚波长谐振模式的Q因子。
The high-Q {\it subwavelength} resonances in an isolated dielectric disk modes can be achieved by avoided crossing (anticrossing) of the nonorthogonal TE resonances under variation of the aspect ratio as it was reported by Rybin {\it et al} [Phys. Rev. Lett. 119, 243901 (2017)]. Traversing over two parameters, the aspect ratio and the distance between two disks, enhances the Q factor by several times compared to the case of the former case of one-parametric avoided crossing in the isolated disk. Therefore successive two-parametric avoided crossing gives multiplicative gain in the Q-factor as it was expected. However if for the single disk its orthogonal resonant modes do not undergo avoided crossing, a presence of the second disk gives removes this restriction and gives rise to the avoided crossing of these modes that enhances the $Q$ factor by two orders in magnitude compared to the case of single disk. Respectively the multipolar decomposition of the anti-bonding resonant mode demonstrates conversion from lower to higher orders of the multipole modes similar to that as shown by Chen {\it et al} [Laser&PhotonicsReviews 13, 1900067 (2019)]. These results are interpreted by that the field configuration at the maximal conversion becomes close to the Mie resonant mode with high orbital momentum in equivalent sphere. For m=1 the resonant modes leakage into both type continua that substantially lowers the Q-factor of the subwavelength resonant modes.