In-fibre Fabry-Pérot microresonator with 100 million Q-factor

Author(s):  
E. Obrzud ◽  
S. Lecomte ◽  
T. Herr
Keyword(s):  
Q Factor ◽  
Photonics ◽  
2019 ◽  
Vol 6 (1) ◽  
pp. 27 ◽  
Author(s):  
Kevin Shortiss ◽  
Maryam Shayesteh ◽  
William Cotter ◽  
Alison Perrott ◽  
Mohamad Dernaika ◽  
...  

Optical injection locking has been demonstrated as an effective filter for optical communications. These optical filters have advantages over conventional passive filters, as they can be used on active material, allowing them to be monolithically integrated onto an optical circuit. We present an experimental and theoretical study of the optical suppression in injection locked Fabry–Pérot and slotted Fabry–Pérot lasers. We consider both single frequency and optical comb injection. Our model is then used to demonstrate that improving the Q factor of devices increases the suppression obtained when injecting optical combs. We show that increasing the Q factor while fixing the device pump rate relative to threshold causes the locking range of these demultiplexers to asymptotically approach a constant value.


2010 ◽  
Vol 17 (4) ◽  
pp. 543-552 ◽  
Author(s):  
Maurine Malak ◽  
Nicolas Pavy ◽  
Frédéric Marty ◽  
Elodie Richalot ◽  
Ai-Qun Liu ◽  
...  
Keyword(s):  
Q Factor ◽  
High Q ◽  

1969 ◽  
Vol 47 (5) ◽  
pp. 515-519 ◽  
Author(s):  
J. H. Williamson ◽  
S. S. Medley

The frequency response of the laser interferometer is shown not to be limited by the Q-factor of the external resonator. However, at high fringing rates, the familiar Fabry–Perot fringes develop subsidiary maxima which make the fringe count liable to misinterpretation. This effect is minimized by using an external resonator with large losses. A passive technique employing an eighth-wave plate is described for determining the direction of change in the optical length directly from the fringe pattern.


Micromachines ◽  
2022 ◽  
Vol 13 (1) ◽  
pp. 118
Author(s):  
Jiamin Chen ◽  
Chenyang Xue ◽  
Yongqiu Zheng ◽  
Jiandong Bai ◽  
Xinyu Zhao ◽  
...  

The ideal development direction of the fiber-optic acoustic sensor (FOAS) is toward broadband, a high sensitivity and a large dynamic range. In order to further promote the acoustic detection potential of the Fabry–Pérot etalon (FPE)-based FOAS, it is of great significance to study the acoustic performance of the FOAS with the quality (Q) factor of FPE as the research objective. This is because the Q factor represents the storage capability and loss characteristic of the FPE. The three FOASs with different Q factors all achieve a broadband response from 20 Hz to 70 kHz with a flatness of ±2 dB, which is consistent with the theory that the frequency response of the FOAS is not affected by the Q factor. Moreover, the sensitivity of the FOAS is proportional to the Q factor. When the Q factor is 1.04×106, the sensitivity of the FOAS is as high as 526.8 mV/Pa. Meanwhile, the minimum detectable sound pressure of 347.33 μPa/Hz1/2  is achieved. Furthermore, with a Q factor of 0.27×106, the maximum detectable sound pressure and dynamic range are 152.32 dB and 107.2 dB, respectively, which is greatly improved compared with two other FOASs. Separately, the FOASs with different Q factors exhibit an excellent acoustic performance in weak sound detection and high sound pressure detection. Therefore, different acoustic detection requirements can be met by selecting the appropriate Q factor, which further broadens the application range and detection potential of FOASs.


Author(s):  
J. Krupka ◽  
A. Cwikla ◽  
M. Mrozowski ◽  
R.N. Clarke ◽  
M.E. Tobar

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