用于微波光子振荡器激光稳定的高q光学谐振器

P. Merrer, A. Bouchier, H. Brahimi, Olivier Llopis, G. Cibiel
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引用次数: 2

摘要

为了设计出紧凑、高性能的微波振荡器,研究了新型谐振腔。由于微波范围的波长较长,谐振腔的尺寸本质上是大的。其次,这些谐振器的质量因子现在被限制在约2.105在10 GHz与窃窃廊模式(WGM)蓝宝石谐振器。然而,如果我们使用光波作为射频频率的载体,例如1.5 μ m激光,就有可能解决这些困难。谐振器变为光学谐振器,由于波长短而具有低维数。光学谐振器产生具有微波间隔的光学频率梳。该梳的每个模式都具有光学Q因子(Qopt)和等效RF Q因子(QRF)的特征。QRF是Qopt与RF光频比的乘积。在1.55µm时,该频率比在20GHz时约为104,Qopt必须至少等于108才能在20GHz时获得比微波谐振器更好的质量。本文介绍了几种不同的高q光谐振器,并介绍了其中一种高q光谐振器在微波光子振荡器中的应用。
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High-Q optical resonators for laser stabilization in microwave photonics oscillators
New resonators are investigated in order to design compact and high performances microwave oscillators. Because of long wavelengths in microwave range, dimensions of resonators are intrinsically large. Secondly, the quality factor of these resonators is now limited to about 2.105 at 10 GHz with whispering gallery modes (WGM) sapphire resonators. Nevertheless, it is possible to solve these difficulties if we use optical waves as a carrier for the RF frequencies, for example a 1.5 µm-laser. Resonators become optical ones, with low dimensions due to short wavelengths. The optical resonator creates an optical frequency comb with microwave spacing. Each mode of this comb is characterized by an optical Q factor (Qopt) and an equivalent RF Q factor (QRF). QRF is the product of Qopt and the RF to optical frequencies ratio. At 1.55 µm, this frequency ratio is about 104 at 20GHz and Qopt must be at least equal to 108 to obtain a quality at 20 GHz better than the microwave resonators. We present different high-Q optical resonators and an application of one of them to microwave photonics oscillators.
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