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Journal articles on the topic 'Optical ring cavity'

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Author: Grafiati

Published: 10 March 2023

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1

Jin, Miao, Jiang Yan-Yi, Fang Su, Bi Zhi-Yi, and Ma Long-Sheng. "Vibration insensitive optical ring cavity." Chinese Physics B 18, no. 6 (June 2009): 2334–39. http://dx.doi.org/10.1088/1674-1056/18/6/037.

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2

Xiaobing Xie, Xiaobing Xie, Xiaolei Zhu Xiaolei Zhu, Shiguang Li Shiguang Li, Xiuhua Ma Xiuhua Ma, Xiao Chen Xiao Chen, Yanguang Sun Yanguang Sun, Huaguo Zang Huaguo Zang, Jiqiao Liu Jiqiao Liu, and Weibiao Chen Weibiao Chen. "Injection-seeded single frequency 2.05 μm output by ring cavity optical parametric oscillator." Chinese Optics Letters 15, no. 9 (2017): 091902. http://dx.doi.org/10.3788/col201715.091902.

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3

Kubstrup, Christian, and Erik Mosekilde. "Bifurcation structure of an optical ring cavity." Physica Scripta T67 (January 1, 1996): 167–75. http://dx.doi.org/10.1088/0031-8949/1996/t67/033.

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4

Gong, Shang-qing, Shao-hua Pan, and Guo-zhen Yang. "Optical bistability in a dye-ring cavity." Physical Review A 45, no. 9 (May 1, 1992): 6655–58. http://dx.doi.org/10.1103/physreva.45.6655.

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5

Petnikova, V. M., and Vladimir V. Shuvalov. "Optimal feedback in efficient ring double-cavity optical parametric oscillators." Quantum Electronics 40, no. 7 (September 10, 2010): 624–28. http://dx.doi.org/10.1070/qe2010v040n07abeh014311.

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6

Telfah, Hamzeh, Anam C. Paul, and Jinjun Liu. "Aligning an optical cavity: with reference to cavity ring-down spectroscopy." Applied Optics 59, no. 30 (October 16, 2020): 9464. http://dx.doi.org/10.1364/ao.405189.

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7

Loock, Hans-Peter, Jack A. Barnes, Gianluca Gagliardi, Runkai Li, Richard D. Oleschuk, and Helen Wächter. "Absorption detection using optical waveguide cavities." Canadian Journal of Chemistry 88, no. 5 (May 2010): 401–10. http://dx.doi.org/10.1139/v10-006.

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Cavity ring-down spectroscopy is a spectroscopic method that uses a high quality optical cavity to amplify the optical loss due to the light absorption by a sample. In this presentation we highlight two applications of phase-shift cavity ring-down spectroscopy that are suited for absorption measurements in the condensed phase and make use of waveguide cavities. In the first application, a fiber loop is used as an optical cavity and the sample is introduced in a gap in the loop to allow absorption measurements of nanoliters of solution at the micromolar level. A second application involves silica microspheres as high finesse cavities. Information on the refractive index and absorption of a thin film of ethylene diamine on the surface of the microresonator is obtained simultaneously by the measurements of the wavelength shift of the cavity mode spectrum and the change in optical decay time, respectively.

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8

Levenson, M. D., B. A. Paldus, T. G. Spence, C. C. Harb, J. S. Harris Jr, and R. N. Zare. "Optical heterodyne detection in cavity ring-down spectroscopy." Chemical Physics Letters 290, no. 4-6 (July 1998): 335–40. http://dx.doi.org/10.1016/s0009-2614(98)00500-4.

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9

Burkart, Johannes, Daniele Romanini, and Samir Kassi. "Optical feedback frequency stabilized cavity ring-down spectroscopy." Optics Letters 39, no. 16 (August 6, 2014): 4695. http://dx.doi.org/10.1364/ol.39.004695.

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10

Hamilton, D. J., M. G. D. Nix, S. G. Baran, G. Hancock, and A. J. Orr-Ewing. "Optical feedback cavity-enhanced absorption spectroscopy (OF-CEAS) in a ring cavity." Applied Physics B 100, no. 2 (November 12, 2009): 233–42. http://dx.doi.org/10.1007/s00340-009-3811-6.

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11

Gao, Feilong, Yiyan Xie, Yiran Wang, Xiancui Su, Guoru Li, Santosh Kumar, and Bingyuan Zhang. "Terahertz parametric oscillator with a rhombic ring-cavity." Japanese Journal of Applied Physics 61, no. 4 (March 17, 2022): 040901. http://dx.doi.org/10.35848/1347-4065/ac5948.

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Abstract Terahertz parametric oscillator (TPO) with a rhombic ring-cavity is demonstrated. The oscillating cavity is composed of three mirrors and the terahertz emitting-surface. Terahertz frequency can be tuned from 0.9 THz to 2.9 THz just by shifting the position of a cavity mirror. Under a certain round-trip optical length of the Stokes beam, the pump beam size can be larger in the rhombic ring-cavity TPO than that in the conventional resonant-cavity TPO. The maximum terahertz pulse energy in the rhombic ring-cavity TPO is 3.21 μJ, which is about 3 times higher than that in the conventional resonant-cavity TPO.

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12

Dong Hewei, 董贺伟, 郭瑞民 Guo Ruimin, 崔文超 Cui Wenchao, and 李东 Li Dong. "Cavity Ring-Down Spectroscopy Based on Folded Cavity." Chinese Journal of Lasers 47, no. 3 (2020): 0311001. http://dx.doi.org/10.3788/cjl202047.0311001.

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13

Luo, Min, Wei Cao, and Haiyan Chen. "Effect of SESAM on continuous-wave multi-wavelength fiber ring-cavity laser with semiconductor optical amplifier." International Journal of Modern Physics B 33, no. 09 (April 10, 2019): 1950076. http://dx.doi.org/10.1142/s0217979219500760.

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The effect of semiconductor saturable absorber mirror (SESAM) on continuous-wave multi-wavelength fiber ring-cavity laser with semiconductor optical amplifier (SOA) is experimentally demonstrated. The evolutionary process of multi-wavelength oscillation and the decrease of oscillating mode number caused by an SESAM are discussed. It’s found that the free oscillating mode number of the multi-wavelength fiber ring-cavity laser with SOA can be upto three, and the lasing wavelengths are 1573.8 nm, 1578.09 nm and 1582.37 nm, respectively. When a SESAM is inserted in the fiber ring-cavity, it narrows the amplified spontaneous emission (ASE) spectrum of the SOA, and the oscillating mode number of the multi-wavelength fiber ring-cavity lasers with SOA decreases to two, a stable dual-wavelength lasing at 1560.91 nm and 1564.12 nm is obtained.

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14

Tan, Zhongqi, and Xingwu Long. "A Developed Optical-Feedback Cavity Ring-Down Spectrometer and its Application." Applied Spectroscopy 66, no. 5 (May 2012): 492–95. http://dx.doi.org/10.1366/11-06291.

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A developed spectrometer based on optical-feedback cavity ring-down spectroscopy (OF-CRDS) has been demonstrated with a distributed feedback laser diode and a V-shaped glass ceramic cavity. The laser is coupled to the V-shaped cavity, which creates an absorption path length greater than 2.8 km, and resonance between the laser frequency and the cavity modes is realized by modulating the cavity length instead of tuning the laser wavelength to obtain a higher resolution. A noise-equivalent absorption coefficient of ∼2.6 × 10−8 cm−1Hz−1/2 (1σ) is determined with spectral resolution of ∼0.003 cm−1 and spectral range of 1.2 cm−1. As an application example, the absorption spectrum measurement of water vapor in the spectral range of 6590.3∼6591.5 cm−1 is demonstrated with this spectrometer.

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15

Dubroeucq, Romain, and Lucile Rutkowski. "Optical frequency comb Fourier transform cavity ring-down spectroscopy." Optics Express 30, no. 8 (April 6, 2022): 13594. http://dx.doi.org/10.1364/oe.454775.

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16

Luo, Min, Wei Cao, and Haiyan Chen. "Fiber ring-cavity laser based on semiconductor optical amplifier." International Journal of Modern Physics B 32, no. 24 (September 13, 2018): 1850266. http://dx.doi.org/10.1142/s0217979218502661.

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A fiber ring-cavity laser based on InP/InGaAsP multi-quantum wells semiconductor optical amplifier is proposed and experimentally demonstrated. The laser uses InP/InGaAsP multi-quantum as well as the gain medium and fiber Bragg grating as the wavelength selector. It’s demonstrated that the center wavelength of the output amplified spontaneous emission spectrum for the InP/InGaAsP multiple-quantum wells appears blue shift when its injection current increases. A lasing at central wavelength of 1549.66 nm with the maximum output power of 1.524 mW is obtained with electro-optical efficiency of 1.1% at injection current of 220 mA and the fiber Bragg grating operating temperature of 23[Formula: see text]C. The threshold injection current of the laser is 78 mA. When the operating temperature of fiber Bragg grating increases from 8[Formula: see text]C to 28[Formula: see text]C, the center wavelength of output laser increases from 1549.27 to 1549.59 nm. It shows that the laser has good temperature stability.

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17

Müller, Thomas, Kenneth B. Wiberg, and Patrick H. Vaccaro. "An optical mounting system for cavity ring-down polarimetry." Review of Scientific Instruments 73, no. 3 (March 2002): 1340–42. http://dx.doi.org/10.1063/1.1448906.

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18

Jiangfeng Xu. "Optical Mode Splitting in Ring-Shaped Hollow Bragg Cavity." IEEE Photonics Technology Letters 27, no. 2 (January 15, 2015): 165–68. http://dx.doi.org/10.1109/lpt.2014.2363881.

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19

Williamson, Andrew P., and Johannes Kiefer. "Polarization-controlled optical ring cavity (PORC) tunable pulse stretcher." Optics Communications 372 (August 2016): 98–105. http://dx.doi.org/10.1016/j.optcom.2016.03.091.

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20

Tanimoto, Hirokazu, Tatuya Matuo, and Yoshinobu Maeda. "Cavity Ring-Down Characteristic Using Reflective Semiconductor Optical Amplifier." IEEJ Transactions on Sensors and Micromachines 130, no. 6 (2010): 253–54. http://dx.doi.org/10.1541/ieejsmas.130.253.

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21

Tanimoto, Hirokazu, Tatuya Matuo, and Yoshinobu Maeda. "Cavity Ring-Down Spectroscopy Using Reflective Semiconductor Optical Amplifier." IEEJ Transactions on Sensors and Micromachines 131, no. 8 (2011): 292–95. http://dx.doi.org/10.1541/ieejsmas.131.292.

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22

Cao Lin, Wang Chun-Mei, Chen Yang-Qin, and Yang Xiao-Hua. "Theoretical investigation of optical heterodyne cavity ring down spectroscopy." Acta Physica Sinica 55, no. 12 (2006): 6354. http://dx.doi.org/10.7498/aps.55.6354.

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23

Tanimoto, Hirokazu, Tatuya Matuo, and Yoshinobu Maeda. "Cavity ring-down spectroscopy using reﬂective semiconductor optical ampliﬁer." Electronics and Communications in Japan 96, no. 5 (April 11, 2013): 37–41. http://dx.doi.org/10.1002/ecj.11378.

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24

Meng, Xiang Ran, Yu Zhao, Xiao Qian Wang, Peng Fei Xu, Wen Dong Zhang, and Shu Bin Yan. "The Effect of Vibration Noise for Cavity Ring Down Time Extraction." Key Engineering Materials 562-565 (July 2013): 1402–7. http://dx.doi.org/10.4028/www.scientific.net/kem.562-565.1402.

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A continue-wave cavity ring down experimental system is established surrounding the micro-sphere cavity. In the experiments of measuring micro-spheres cavity quality factor (Q) upon the system, it is found that photoelectric detectors with different response characteristic have different response to the optical signal which is shut off rapidly. The vibration noise caused by changes of external environment, meanwhile, can be transformed following the change of photoelectric detector properties. With the build of photoelectric detector response model, the mean-square deviation of repeated experiments under the same conditions is used for charactering level of the error caused by vibration noise. The influence of vibration noise to photoelectric detector is discussed in detail, and further analyzes the effect for the cavity ring down time extraction. Then the optimal photoelectric detector (Newfocus1434, 15V/W) is selected to optimize the experimental system. The level of error caused by vibration noise has been decreased from 0.191ns to 1.562ps. Finally, the Q value of micro-sphere cavity is calculated according to fitted value of cavity ring down time, and the experimental correctness is verified by the line-width law.

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25

BRUNEL, M., and F. SANCHEZ. "OPTICAL LIMITING INDUCED BY CAVITY FEEDBACK IN A RESONANT DENSE MEDIUM." Journal of Nonlinear Optical Physics & Materials 09, no. 03 (September 2000): 261–68. http://dx.doi.org/10.1142/s0218863500000297.

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We investigate the optical limiting behavior exhibited by a resonant dense medium when inserted in a ring cavity. The influence of the cavity parameters, the atomic frequency detuning and the density of atoms are determined.

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26

Wang, Xing-Ping, Gang Zhao, Kang Jiao, Bing Chen, Rui-Feng Kan, Jian-Guo Liu, and Wei-Guang Ma. "Uncertainty of optical feedback linear cavity ringdown spectroscopy." Acta Physica Sinica 71, no. 12 (2022): 124201. http://dx.doi.org/10.7498/aps.70.20220186.

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Cavity ring-down spectroscopy (CRDS) is a highly sensitive molecular absorption spectroscopic technology, which has been widely used in mirror reflectance measurement, atmospheric trace gas detection, molecular precision spectroscopy and other fields. It deduces the intracavity absorption by measuring the rapid variation of the ringdown signal. As a result, detector with high linearity, broad bandwidth and low electrical noise is indispensable. Additionally, owing to the large noise in laser frequency, low laser-to-cavity coupling efficiency is obtained. Consequently, the cavity transmission is faint, which deteriorates the detection sensitivity. Optical feedback can address this problem by locking the laser to the cavity longitudinal mode. Then, the laser frequency noise is suppressed and hence better detection sensitivity is expected. Optical feedback CRDS with V-shape cavity has been widely studied. Compared with Fabry-Perot cavity, this cavity geometry is very sensitive to mechanical vibration and possesses low degree of fineness due to an additional mirror. In this paper, optical feedback linear cavity ring-down spectroscopy based on a Fabry-Perot cavity with a degree of fineness of 7800 is presented. The principle of the combination of optical feedback and linear cavity is explained from the perspective of the light phase, which shows that the reflection will not generate efficient optical feedback if the feedback phase is appropriately controlled and laser to cavity locking can be therefore realized. And then, the factors influencing the stability of ring-down signal are analyzed, including the feedback ratio, the trigger voltage for the ringdown event, and the distance between the light spot and the detector center. The experimental results show that a superior fractional uncertainty of the empty ringdown time of 0.026% can be obtained with a low feedback rate (3% FSR), a high ringdown signal trigger threshold (90% cavity mode amplitude) and superposition of the light spot with the detector center. With Allan variance analysis, the white noise response of 1.56 × 10<sup>–9</sup> cm<sup>–1</sup>/ Hz<sup>–1/2</sup> and the detection sensitivity of 1.29 × 10<sup>–10</sup> cm<sup>–1</sup> for trace gas detection can be achieved in an integration time of 180 s, corresponding to the lowest CH<sub>4</sub> concentration detection of 0.35 ppb at 6046.9 cm<sup>–1</sup>. This robust spectroscopic technique paves the way for constructing high-sensitive and stable-cavity based instrument for trace gas detection.

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27

Duraev, V. P., and S. V. Medvedev. "Fibre ring cavity semiconductor laser." Quantum Electronics 43, no. 10 (October 31, 2013): 914–16. http://dx.doi.org/10.1070/qe2013v043n10abeh015256.

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28

Wang, Xiao Qian, Shu Bin Yan, Ke Zhen Ma, Peng Fei Xu, and Wen Dong Zhang. "A Novel Noise Resistance Optical Accelerometer Based on Micro-Ring Resonant Cavity." Key Engineering Materials 562-565 (July 2013): 232–36. http://dx.doi.org/10.4028/www.scientific.net/kem.562-565.232.

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To meet a high-precision accelerometer resistance of temperature, humidity and other external noise, a new multi-ring cascade optical accelerometer structure is designed. The micro-ring resonator on the cantilever beam based on the photo-elastic effect and the contrast are fabricated with the same manufacturing process and size, which can effectively meet the consistency of the contrast and test micro-ring resonator on the cantilever. The one resonance point curve will split into two under the acceleration, thus the acceleration value can be obtained by detecting the wavelength of the two resonant points. By testing the cascade race-track shaped micro-ring resonator at different temperatures, the Q=104, the test requirement of cascade race-track shaped micro-ring accelerometer in different environments is greatly met. The design can be widely applied to the occasions of penetration system with high impact, strong vibration and so on. And the anti-noise and anti-jamming features of the integrated miniaturized high-sensitivity MOEMS sensors are realized.

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29

Aguilar, E., S. Srepanov, and E. Hernandez. "Optical-fiber ring cavity with saturable rare-earth-doped fiber." Suplemento de la Revista Mexicana de Física 2, no. 1 Jan-Mar (March 31, 2021): 11–18. http://dx.doi.org/10.31349/suplrevmexfis.2.1.11.

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Resonance properties of the all-fiber ring cavity filled with nonlinear material - saturable rare-earth-doped fiber are analyzed and experimentally investigated. Unlike the earlier investigated erbium-doped fiber at 1550nm where the optical absorption photo-induced change (saturation) is observed only, the ytterbium-doped fiber at 1064nm demonstrates the saturation of the refractive index mainly. For this configuration we report experimental observation of the optical bistability and hysteresis in the transmitted output light at the 10mW-scale incident light power. The experimental results are in qualitative agreement with the theoretical analysis that takes into account the saturation of both parameters: the optical absorption and the refractive index of the doped fiber. The reported results seem promising for applications in high-sensitivity interferometric configurations at 1064nm operation wavelength.

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30

Chen, Su, Weixiang Hu, Yang Xu, Yu Cai, Zhiqiang Wang, and Zuxing Zhang. "Mode-locked pulse generation from an all-FMF ring laser cavity." Chinese Optics Letters 17, no. 12 (2019): 121405. http://dx.doi.org/10.3788/col201917.121405.

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31

Tan Zhongqi, 谭中奇, 吴素勇 Wu Suyong, 刘贱平 Liu Jianping, 杨开勇 Yang Kaiyong, and 龙兴武 Long Xingwu. "Spectrum data processing in optical-feedback cavity ring-down spectroscopy." High Power Laser and Particle Beams 26, no. 10 (2014): 101006. http://dx.doi.org/10.3788/hplpb20142610.101006.

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32

Bincheng Li, 李斌成, 曲折超 Zhechao Qu, 韩艳玲 Yanling Han, 高丽峰 Lifeng Gao, and 李凌辉 Linghui Li. "Optical feedback cavity ring-down technique for high reflectivity measurement." Chinese Optics Letters 8, S1 (2010): 94–98. http://dx.doi.org/10.3788/col201008s1.0094.

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33

Candiani, Alessandro, Michele Sozzi, Annamaria Cucinotta, Stefano Selleri, Rosanna Veneziano, Roberto Corradini, Rosangela Marchelli, Paul Childs, and Stavros Pissadakis. "Optical Fiber Ring Cavity Sensor for Label-Free DNA Detection." IEEE Journal of Selected Topics in Quantum Electronics 18, no. 3 (May 2012): 1176–83. http://dx.doi.org/10.1109/jstqe.2011.2166110.

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34

Yilmaz, Arzu, Simon Schuster, Philip Wolf, Dag Schmidt, Max Eisele, Claus Zimmermann, and Sebastian Slama. "Optomechanical damping of a nanomembrane inside an optical ring cavity." New Journal of Physics 19, no. 1 (January 31, 2017): 013038. http://dx.doi.org/10.1088/1367-2630/aa55ee.

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35

Möller, M., L. M. Hoffer, G. L. Lippi, T. Ackemann, A. Gahl, and W. Lange. "Fabry-Pérot and ring cavity configurations and transverse optical patterns." Journal of Modern Optics 45, no. 9 (September 1998): 1913–26. http://dx.doi.org/10.1080/09500349808231710.

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36

Möller, M., L. M. Hoffer, G. L. Lippi, T. Ackemann, A. Gahl, and W. Lange. "Fabry-Pérot and ring cavity configurations and transverse optical patterns." Journal of Modern Optics 45, no. 9 (September 1, 1998): 1913–26. http://dx.doi.org/10.1080/095003498150781.

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37

Chen, Hua-Jun, Bao-Cheng Hou, and Jian-Yong Yang. "Controllable coherent optical response in a ring cavity optomechanical system." Physica E: Low-dimensional Systems and Nanostructures 125 (January 2021): 114394. http://dx.doi.org/10.1016/j.physe.2020.114394.

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38

Śmigaj, Wojciech, Liubov Magdenko, Javier Romero-Vivas, Sébastien Guenneau, Béatrice Dagens, Boris Gralak, and Mathias Vanwolleghem. "Compact optical circulator based on a uniformly magnetized ring cavity." Photonics and Nanostructures - Fundamentals and Applications 10, no. 1 (January 2012): 83–101. http://dx.doi.org/10.1016/j.photonics.2011.07.004.

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39

Jun, Zhu, Qin Liuli, and Song shuxiang. "Surface plasmon resonance demodulation by optical ring-down cavity technology." Optik 127, no. 3 (February 2016): 1207–12. http://dx.doi.org/10.1016/j.ijleo.2015.10.090.

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40

Chiou, Arthur E. T., and Pochi Yeh. "Scaling and rotation of optical images using a ring cavity." Applied Optics 29, no. 11 (April 10, 1990): 1584. http://dx.doi.org/10.1364/ao.29.001584.

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41

Li, Ling, Jianmin Chen, Hui Chen, Xin Yang, Yong Tang, and Renyi Zhang. "Monitoring optical properties of aerosols with cavity ring‐down spectroscopy." Journal of Aerosol Science 42, no. 4 (April 2011): 277–84. http://dx.doi.org/10.1016/j.jaerosci.2011.02.001.

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42

Passos, D. J., S. O. Silva, J. R. A. Fernandes, M. B. Marques, and O. Frazão. "Fiber cavity ring-down using an optical time-domain reflectometer." Photonic Sensors 4, no. 4 (August 9, 2014): 295–99. http://dx.doi.org/10.1007/s13320-014-0205-0.

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43

Wang, Fei, Guang-Qiong Xia, and Zheng-Mao Wu. "All-optical frequency multiplication/recovery based on a semiconductor optical amplifier ring cavity." Optics Communications 257, no. 2 (January 2006): 334–39. http://dx.doi.org/10.1016/j.optcom.2005.07.074.

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44

Takahashi, Yoshitaka, Yudai Fukaya, and Sho Takahashi. "Orthogonal Dual-Frequency SOA-Fiber Laser." Key Engineering Materials 596 (December 2013): 129–33. http://dx.doi.org/10.4028/www.scientific.net/kem.596.129.

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In order to develop a new orthogonal dual-frequency laser, we studied a fiber ring laser using a SOA (semiconductor optical amplifier) and aim to apply it to a novel light source for optical heterodyne interferometry. The frequency difference was generated by a linear or circular birefringent medium inserted into the ring cavity. To obtain heterodyne signal optical and electrical filters were introduced.

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45

Kranz, Michael, Tracy Hudson, Brian Grantham, and Michael Whitley. "Optical Cavity Interrogation for MEMS Accelerometers." Additional Conferences (Device Packaging, HiTEC, HiTEN, and CICMT) 2015, DPC (January 1, 2015): 001649–70. http://dx.doi.org/10.4071/2015dpc-wp34.

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MEMS accelerometers utilizing electrostatic, piezoelectric, and magnetic proof mass displacement readout approaches have achieved success in both commercial- and defense-related applications. However, there is a desire for improved acceleration resolution suitable for navigation-grade applications. Optical readout of mechanical displacements has demonstrated high levels of resolution in macro-scale applications including precision movement and placement systems. In addition, optical techniques are common in high performance inertial sensors such as fiber optic gyros and ring laser gyros. Incorporating optical readout approaches into MEMS acceleration devices may yield sufficient resolution to achieve navigation-grade performance. Therefore, the U.S. Army AMRDEC is developing MEMS accelerometers based on optical cavity resonance readout. In the device, an optical cavity is formed between a MEMS proof mass and a reference reflector. A tunable laser excites the cavity on the edge of its resonance peak. Small displacements of the cavity from its rest position are detected by frequency shifts of the resonance, leading to high-resolution proof mass displacement detection and therefore high acceleration resolutions. This paper will present modeling associated with the design concept, as well predictions of device geometries and performance with the goal of achieving less than 1 micro-g bias instability and a velocity random walk of better than 0.2 micro-g/rt.Hz.

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46

Singh, Alok K., Lal Muanzuala, Atanu K. Mohanty, and Vasant Natarajan. "Optical frequency metrology with an Rb-stabilized ring-cavity resonator—study of cavity-dispersion errors." Journal of the Optical Society of America B 29, no. 10 (September 12, 2012): 2734. http://dx.doi.org/10.1364/josab.29.002734.

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47

Zhadnov, N. O., and A. V. Masalov. "Temperature-compensated optical cavities for laser frequency stabilization." Laser Physics Letters 20, no. 3 (January 19, 2023): 030001. http://dx.doi.org/10.1088/1612-202x/acb1ad.

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Abstract We propose a method for thermal expansion compensation of reference monolithic optical cavities for laser frequency stabilization. Two schemes of optical cavities are considered: a Fabry–Perot interferometer with a crimp ring and a whispering-gallery-mode cavity with a clamp. In each scheme, thermal expansion compensation is achieved due to the strained connection of the cavity with an element made of a material with a high coefficient of thermal expansion. The temperature range of the cavities’ optical length stabilization is estimated.

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48

Liang, Tsair-Chun, and Chun-Ting Chen. "Investigation of Dispersion and Performance Based on Ring Cavity by Birefringent Interleaver for DWDM Transmission Systems." Mathematical Problems in Engineering 2013 (2013): 1–5. http://dx.doi.org/10.1155/2013/740412.

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We theoretically investigate a 25 GHz multichannel filter based on ring cavity birefringent optical interleaver for dense wavelength division multiplexing (DWDM) transmission systems. The simulation tool used in this work is the Advanced System Analysis Program (ASAP) optical modeling software. We improve the dispersion performance by employingλ/6 andλ/4 wave plates as birefringent compensators for interleavers. The new structure exhibits a high performance with nearly zero ripple, a channel isolation greater than 102 dB, and a passband utilization of 86% within the C-band. The research results illustrate that our modified scheme can improve the dispersion of more than 76.6% in comparison with the previous studies of optical interleaver with birefringent crystal and ring cavity structures.

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Jachpure, Deeksha, and R. Vijaya. "Saturable absorption and its consequent effects in bistable erbium-doped fiber ring laser." Journal of Optics 24, no. 2 (January 5, 2022): 024007. http://dx.doi.org/10.1088/2040-8986/ac41d6.

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Abstract The linear absorption in erbium-doped fiber (EDF) contributes to its excellent role in EDF amplifiers and lasers. A nonlinear optical contribution in the absorption of EDF is responsible for optical bistable action when it is present in a laser cavity. To quantify this effect, the variation of absorption coefficient is measured at different signal powers at multiple wavelengths in the C-band for different EDF lengths, and saturable absorption parameters such as the saturation power are extracted. Then the modification in the output characteristics of EDF ring laser with change in fiber length and in the presence of self-induced saturable absorption effect within the gain medium, which leads to optical bistability, is measured. By comparing the measured parameters obtained from saturable absorption in EDF and optical bistability in EDF ring laser, we estimated the length of the gain medium which acts as the saturable absorber inside the cavity of the laser. This is useful in constructing bistable lasers with optimized conditions. The temporal evolution of cavity loss and gain with the intra-cavity power and up- and down-thresholds helps in understanding why the down-threshold will be lesser than the up-threshold in bistable laser systems.

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50

Caglayan, Humeyra, Irfan Bulu, Marko Loncar, and Ekmel Ozbay. "Cavity formation in split ring resonators." Photonics and Nanostructures - Fundamentals and Applications 6, no. 3-4 (December 2008): 200–204. http://dx.doi.org/10.1016/j.photonics.2008.09.001.

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