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Ultra-high-Q toroid microcavity on a chip

机译:芯片上的超高Q环形微腔

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The circulation of light within dielectric volumes enables storage of optical power near specific resonant frequencies and is important in a wide range of fields including cavity quantum electrodynamics(1,2), photonics(3,4), biosensing(5,6) and nonlinear optics(7-9). Optical trajectories occur near the interface of the volume with its surroundings, making their performance strongly dependent upon interface quality. With a nearly atomic-scale surface finish, surface-tension-induced microcavities such as liquid droplets or spheres(10-13) are superior to all other dielectric microresonant structures when comparing photon lifetime or, equivalently, cavity Q factor. Despite these advantageous properties, the physical characteristics of such systems are not easily controlled during fabrication. It is known that wafer-based processing(14) of resonators can achieve parallel processing and control, as well as integration with other functions. However, such resonators-on-a-chip suffer from Q factors that are many orders of magnitude lower than for surface-tension-induced microcavities, making them unsuitable for ultra-high-Q experiments. Here we demonstrate a process for producing silica toroid-shaped microresonators-on-a-chip with Q factors in excess of 100 million using a combination of lithography, dry etching and a selective reflow process. Such a high Q value was previously attainable only by droplets or microspheres and represents an improvement of nearly four orders of magnitude over previous chip-based resonators. [References: 23]
机译:介电体中光的循环能够在特定的谐振频率附近存储光功率,并且在包括腔量子电动力学(1,2),光子学(3,4),生物传感(5,6)和非线性在内的广泛领域中都很重要光学(7-9)。光学轨迹出现在体积与周围环境的界面附近,因此其性能在很大程度上取决于界面质量。在比较光子寿命或等效的腔Q因子时,由于具有接近原子级的表面光洁度,表面张力诱导的微腔(如液滴或球体)(10-13)优于所有其他介电微谐振结构。尽管具有这些有利的特性,但是在制造期间不容易控制这种系统的物理特性。众所周知,基于晶片的谐振器处理(14)可以实现并行处理和控制,以及与其他功能的集成。但是,这种片上谐振器的Q因子比表面张力引起的微腔要低很多数量级,这使其不适用于超高Q实验。在这里,我们展示了一种结合光刻,干法刻蚀和选择性回流工艺生产Q值超过1亿的硅环形微片谐振器的工艺。如此高的Q值以前只能通过液滴或微球获得,并且比以前的基于芯片的谐振器提高了近四个数量级。 [参考:23]

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