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High q-factor distributed bragg reflector resonators with reflectors of arbitrary thickness

机译:具有任意厚度的反射器的高q因数分布式布拉格反射器谐振器

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The Bragg reflection technique improves the Q-factor of a resonator by reducing conductor and dielectric losses. This is achieved by designing a low-loss inner resonant region (usually free space) surrounded by an outer anti-resonant region made of distributed Bragg reflector layers. In this paper we develop a simple non-Maxwellian model and apply it to design three distinct cylindrical Bragg resonators based on the same set of single-crystal sapphire plates and rings by changing only the dimension of the cavity that supports the structure. To accomplish this, the simple model allows an arbitrary thickness for either the horizontal or the cylindrical dielectric reflectors by relaxing the condition that they must be lambda4 thick. The model also allows for higher-order field variations in both the resonant and the anti-resonant regions. The resonators were constructed and experimental results were compared with the simple model and the rigorous method of lines analysis. For the fundamental mode, an unloaded Q-factor of 234,000 at 9.7 GHz was obtained. This is larger than that for a whispering gallery mode resonator. The resonator also exhibited a greatly reduced spurious mode density when compared to an overmoded whispering gallery mode resonator.
机译:布拉格反射技术通过减少导体和介电损耗来改善谐振器的Q因子。这是通过设计一个低损耗的内部谐振区域(通常是自由空间)来实现的,该区域被由分布的布拉格反射器层组成的外部反谐振区域包围。在本文中,我们开发了一个简单的非麦克斯韦模型,并通过仅改变支撑结构的空腔尺寸,将其应用于基于同一组单晶蓝宝石板和环设计三个不同的圆柱形布拉格谐振器。为此,简单的模型通过放宽必须为λ4厚的条件,为水平或圆柱形介电反射器提供任意厚度。该模型还允许谐振和反谐振区域中的高阶场变化。构造了谐振器,并将实验结果与简单模型和严格的线分析方法进行了比较。对于基本模式,在9.7 GHz下获得了234,000的空载Q因子。这比耳语画廊模式谐振器大。与过调制的耳语画廊模式谐振器相比,该谐振器还表现出大大降低的杂散模式密度。

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