掺钕微激光实验及热光效应理论分析

Huibo Fan, Xinrui Chen, Huili Fan, Arui Wang, Ruijuan Chang
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引用次数: 0

摘要

对掺钕二氧化硅环形微腔的超低阈值激光发射进行了理论分析和实验演示,并对该微激光系统中的热光学效应进行了详细分析和补偿。根据耦合模式理论和解析公式推导出了微激光发射的阈值功率和斜率效率,并证明了它们与钕离子浓度和微空腔品质因数的关系。实验中,通过改变腔锥形光纤系统的耦合条件、谐振泵浦波长和泵浦功率,分别获得了波长为 1064 nm 波段、阈值功率低至 1.6 µW 的单模激光器和多模激光器。此外,还实现了 910 nm 波段的单模激光发射,阈值功率约为 108.5 µW。此外,考虑到潜在的应用,由于热光学效应的影响和非谐振泵浦的低斜率效率,用于 1064 nm 波段激光发射的非谐振泵浦的阈值功率为 137 µW。通过在微晶体表面涂覆具有负热光系数的紫外线胶水,从理论上分析了补偿微晶体热光效应的方法,另一方面,这种方法也可用于灵敏度为 -0.138nm/∘C 的高灵敏度温度传感的潜在应用。
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Experimental neodymium-doped microlaser with theoretical analysis of the thermo-optic effect
Ultralow-threshold laser emission from a neodymium-doped silica toroidal microcavity is theoretically analyzed and experimentally demonstrated, along with the detailed analysis and compensation of the thermo-optic effect in this microlaser system. The threshold power and slope efficiency of microlaser emission are derived based on coupled-mode theory and analytic formulas, associated with the demonstration of their dependence on neodymium ion concentration and the quality factor of the microtoroid. In the experiment, a single-mode laser and multi-mode laser with threshold power as low as 1.6 µW at the wavelength of 1064 nm band are obtained via changing the coupling condition of the cavity-tapered fiber system, resonant pump wavelength, and pump power, respectively. The single-mode laser emission at the 910 nm band is also realized with the threshold power of about 108.5 µW. Furthermore, considering the potential application, non-resonant pumping for the laser emission at the 1064 nm band is characterized with threshold power of 137 µW due to the influence of the thermo-optic effect and low slope efficiency of non-resonant pumping. By coating UV-glue with a negative thermo-optic coefficient on the microtoroid surface, the compensation of the thermo-optic effect of the microtoroid is analyzed theoretically, which on the other hand can also be used for the potential application of high-sensitivity temperature sensing with sensitivity of −0.138nm/C.
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