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Artículos de revistas sobre el tema "Optical ring cavity"

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Publicado: 10 de marzo de 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 (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 та ін. "Injection-seeded single frequency 2.05 μm output by ring cavity optical parametric oscillator". Chinese Optics Letters 15, № 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 (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 (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 (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 (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 sili
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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 (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 (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 (2009): 233–42. http://dx.doi.org/10.1007/s00340-009-3811-6.

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11

Gao, Feilong, Yiyan Xie, Yiran Wang, et al. "Terahertz parametric oscillator with a rhombic ring-cavity." Japanese Journal of Applied Physics 61, no. 4 (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
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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 (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 narrow
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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 (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
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15

Dubroeucq, Romain, and Lucile Rutkowski. "Optical frequency comb Fourier transform cavity ring-down spectroscopy." Optics Express 30, no. 8 (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 (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
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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 (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 (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 та Yoshinobu Maeda. "Cavity ring-down spectroscopy using reflective semiconductor optical amplifier". Electronics and Communications in Japan 96, № 5 (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 experi
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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 (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, et al. "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 i
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27

Duraev, V. P., and S. V. Medvedev. "Fibre ring cavity semiconductor laser." Quantum Electronics 43, no. 10 (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 reso
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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 (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
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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, et al. "Optical Fiber Ring Cavity Sensor for Label-Free DNA Detection." IEEE Journal of Selected Topics in Quantum Electronics 18, no. 3 (2012): 1176–83. http://dx.doi.org/10.1109/jstqe.2011.2166110.

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34

Yilmaz, Arzu, Simon Schuster, Philip Wolf, et al. "Optomechanical damping of a nanomembrane inside an optical ring cavity." New Journal of Physics 19, no. 1 (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 (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 (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, et al. "Compact optical circulator based on a uniformly magnetized ring cavity." Photonics and Nanostructures - Fundamentals and Applications 10, no. 1 (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 (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 (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 (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 (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 (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 (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. Incor
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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 (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 (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 result
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49

Jachpure, Deeksha, and R. Vijaya. "Saturable absorption and its consequent effects in bistable erbium-doped fiber ring laser." Journal of Optics 24, no. 2 (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 fibe
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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 (2008): 200–204. http://dx.doi.org/10.1016/j.photonics.2008.09.001.

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