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Journal articles on the topic 'Fabry-Perot resonator'

Author: Grafiati

Published: 4 June 2021

Last updated: 25 July 2025

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1

Nielsen, William Hvidtfelt Padkær, Yeghishe Tsaturyan, Christoffer Bo Møller, Eugene S. Polzik, and Albert Schliesser. "Multimode optomechanical system in the quantum regime." Proceedings of the National Academy of Sciences 114, no. 1 (2016): 62–66. http://dx.doi.org/10.1073/pnas.1608412114.

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We realize a simple and robust optomechanical system with a multitude of long-lived (Q > 107) mechanical modes in a phononic-bandgap shielded membrane resonator. An optical mode of a compact Fabry–Perot resonator detects these modes’ motion with a measurement rate (96 kHz) that exceeds the mechanical decoherence rates already at moderate cryogenic temperatures (10 K). Reaching this quantum regime entails, inter alia, quantum measurement backaction exceeding thermal forces and thus strong optomechanical quantum correlations. In particular, we observe ponderomotive squeezing of the output lig

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2

Nelin, E. A. "Resonator With Reflectors Based on Open-Circuited Stub." Visnyk NTUU KPI Seriia - Radiotekhnika Radioaparatobuduvannia, no. 98 (December 30, 2024): 66–72. https://doi.org/10.20535/radap.2024.98.66-72.

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Introduction. A two-stub resonator is considered as an analogue of a parallel resonant circuit. Another scheme of the resonator is similar to the Fabry-Perot optical resonator, formed by a resonator cavity and two reflectors. In the presented paper it is proposed a combined reflector formed by a stepped-impedance one and an open-circuited stub. Resonators with such reflectors have a higher quality factor Q than those known based on open-circuited stubs and than the Fabry-Perot resonator. 1 Half wavelength resonator. One of the analogues of the Fabry-Perot resonator is a half wavelength section

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3

Matiwane, A., J. Sackey, M. L. Lekala, A. Gibaud, and M. Maaza. "Neutron tunneling in nanostructured systems: isotopical effect." MRS Advances 3, no. 42-43 (2018): 2609–16. http://dx.doi.org/10.1557/adv.2018.228.

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AbstractThis contribution reports, to the best of our knowledge, for the first time on the neutron tunneling phenomenon in nickel isotopes based nanostructured. More accurately, 58Ni-62Ni-58Ni thin films Fabry-Perot resonator configuration exhibited several tunneling resonances. In total, there were 7 tunneling resonances. These tunneling resonances manifest themselves via sharp dips in the total reflection plateau due to quasi-bound states in the nanostructured isotopic based nickel thin film Fabry-Perot resonator.

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4

Lu, Kai, and Kwok Wa Leung. "Differential Fabry–Perot Resonator Antennas." IEEE Transactions on Antennas and Propagation 61, no. 9 (2013): 4438–46. http://dx.doi.org/10.1109/tap.2013.2267196.

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5

Haber, Elad, Mark Douvidzon, Shai Maayani, and Tal Carmon. "A Liquid Mirror Resonator." Micromachines 14, no. 3 (2023): 624. http://dx.doi.org/10.3390/mi14030624.

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We present the first experimental demonstration of a Fabry‒Perot resonator that utilizes total internal reflection from a liquid–gas interface. Our hybrid resonator hosts both optical and capillary waves that mutually interact. Except for the almost perfect reflection by the oil–air interface at incident angles smaller than the critical angle, reflections from the liquid-phase boundary permit optically examining thermal fluctuations and capillary waves at the oil surface. Characterizing our optocapillary Fabry‒Perot reveals optical modes with transverse cross-sectional areas of various shapes

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6

Pilipovich, V. M., V. B. Zalesski, A. I. Kanojka, V. M. Kravchenko, and K. A. Reshikov. "INFRARED RADIATION CONVERTER BASED ON FABRY – PEROT MICRORESONATORS." Proceedings of the National Academy of Sciences of Belarus. Physics and Mathematics Series 54, no. 2 (2018): 234–40. http://dx.doi.org/10.29235/1561-2430-2018-54-2-234-240.

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The method of transformation of information from one spectral range to another based on Fabry – Perot microresonators is offered. The method uses incident radiation of an object as affecting a microresonator material (a microresonator material must absorb this radiation), and visible radiation of the optical part of the spectrum as sensing, or reading radiation (a microresonator material should not absorb this radiation). The absorbed energy of incident radiation leads to a change in a microcavity temperature, which results in a change in the optical base of the resonator. The high sensitivity

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7

Kumar, A. R., V. A. Boychev, Z. M. Zhang та D. B. Tanner. "Fabry-Perot Resonators Built With YBa2Cu3O7−δ Films on Si Substrates". Journal of Heat Transfer 122, № 4 (2000): 785–91. http://dx.doi.org/10.1115/1.1316784.

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Fabry-Perot resonators were built from two superconductive YBa2Cu3O7−δ (YBCO) films separated by a spacer. Each film of 35-nm thickness was deposited on a Si substrate, about 204 μm thick. A slow-scan Michelson interferometer was employed to measure the transmittance of the resonator in the far-infrared frequency region from 10 to 90 cm−1 at temperatures between 10 and 300 K. Measurements showed that in the normal state the peak (or resonant) transmittance decreases as temperature is lowered, whereas in the superconducting state it can increase with decreasing temperature. The transmittance of

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8

Nayak, Chittaranjan, Alireza Aghajamali, and Dipak P. Patil. "Extrinsic magnetized plasma Fabry–Perot resonator." Indian Journal of Physics 93, no. 3 (2018): 401–6. http://dx.doi.org/10.1007/s12648-018-1282-5.

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9

Awwal, Abdul Ahad S., and Mohammad A. Karim. "Low frequency nonlinear fabry-perot resonator." Microwave and Optical Technology Letters 2, no. 3 (1989): 88–91. http://dx.doi.org/10.1002/mop.4650020304.

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10

GROHS, J., F. ZHOU, H. IßLER, and C. KLINGSHIRN. "SELF-OSCILLATIONS OF AN OPTICALLY BISTABLE ELEMENT WITH VERY BROAD HYSTERESIS IN A HYBRID RING CAVITY." International Journal of Bifurcation and Chaos 02, no. 04 (1992): 861–72. http://dx.doi.org/10.1142/s0218127492000483.

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We investigate thermally induced optical nonlinearity of a glass doped with semiconductor quantum dots. With the feedback of a Fabry-Perot resonator this glass shows dispersive optical bistability. The reflected light signal is coupled to a hybrid ring cavity with a round trip time much longer than that of the Fabry-Perot resonator and even longer than the thermal relaxation time of the glass. The self-oscillations occurring for certain input parameters are regular and the appearance of different modes as a function of the light intensity coupled to the resonator is observed. Due to the broad

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11

Bunel, Thomas, Matteo Conforti, Julien Lumeau, et al. "Unexpected phase-locked Brillouin Kerr Frequency comb in fiber Fabry Perot resonators." EPJ Web of Conferences 287 (2023): 07005. http://dx.doi.org/10.1051/epjconf/202328707005.

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12

Choi, Jihoon, and Heeso Noh. "Single-Port Coherent Perfect Loss in a Photonic Crystal Nanobeam Resonator." Nanomaterials 11, no. 12 (2021): 3457. http://dx.doi.org/10.3390/nano11123457.

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We numerically demonstrated single-port coherent perfect loss (CPL) with a Fabry–Perot resonator in a photonic crystal (PC) nanobeam by using a perfect magnetic conductor (PMC)-like boundary. The CPL mode with even symmetry can be reduced to a single-port CPL when a PMC boundary is applied. The boundary which acts like a PMC boundary, here known as a PMC-like boundary, and can be realized by adjusting the phase shift of the reflection from the PC when the wavelength of the light is within the photonic bandgap wavelength range. We designed and optimized simple Fabry–Perot resonator and coupler

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13

Zhao, Yan, Shu-Fang Fu, Hua Li, and Xuan-Zhang Wang. "Bistable transmission of antiferromagnetic Fabry-Perot resonator." Journal of Applied Physics 110, no. 2 (2011): 023512. http://dx.doi.org/10.1063/1.3608043.

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14

Liu, Zhen-guo, Zhi-chen Ge, and Xi-yuan Chen. "Research progress on Fabry-Perot resonator antenna." Journal of Zhejiang University-SCIENCE A 10, no. 4 (2009): 583–88. http://dx.doi.org/10.1631/jzus.a0820546.

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15

Urquhart, Paul. "Transversely coupled fiber Fabry-Perot resonator: theory." Applied Optics 26, no. 3 (1987): 456. http://dx.doi.org/10.1364/ao.26.000456.

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16

NARDUCCI, FRANK, ZONGXIONG YE, and HONG LING. "Laser cooling in a Fabry-Perot resonator." Journal of Modern Optics 49, no. 3-4 (2002): 687–704. http://dx.doi.org/10.1080/09500340110111121.

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17

Poon, Joyce K. S., Philip Chak, John M. Choi, and Amnon Yariv. "Slowing light with Fabry-Perot resonator arrays." Journal of the Optical Society of America B 24, no. 11 (2007): 2763. http://dx.doi.org/10.1364/josab.24.002763.

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18

Burns, Thomas J. "Fabry-Perot confocal resonator optical associative memory." Optical Engineering 32, no. 3 (1993): 469. http://dx.doi.org/10.1117/12.61204.

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19

Ediss, G. A., and P. R. Lawson. "Fabry–Perot resonator diplexer at 230 GHz." IEE Proceedings H Microwaves, Antennas and Propagation 136, no. 5 (1989): 411. http://dx.doi.org/10.1049/ip-h-2.1989.0073.

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20

Lugiato, L. A., and L. M. Narducci. "Nonlinear dynamics in a Fabry-Perot resonator." Zeitschrift f�r Physik B Condensed Matter 71, no. 1 (1988): 129–38. http://dx.doi.org/10.1007/bf01310852.

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21

Richard, J. P., J. J. Hamilton, and Y. Pang. "Fabry-Perot optical resonator at low temperatures." Journal of Low Temperature Physics 81, no. 3-4 (1990): 189–98. http://dx.doi.org/10.1007/bf00682681.

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22

Zhang, Jian-Luo, and John W. Y. Lit. "A symmetric figure-of-eight optical fiber resonator." Canadian Journal of Physics 71, no. 1-2 (1993): 20–24. http://dx.doi.org/10.1139/p93-004.

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A theoretical study is presented of a figure-of-eight optical fiber resonator that has two single-mode couplers. The output intensities of the optical fiber resonator are investigated in terms of the coupling coefficients and losses. The finesse and contrast are discussed. Compared with a transversely coupled fiber Fabry–Perot resonator, this resonator has an all-fiber configuration, and is more easily realized. Compared with a direct-coupling fiber ring resonator, it offers reflected outputs that may be useful in some applications.

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23

Zhang, Shao Jun, Yue Ming Liu, and Xiao Hong Huangfu. "Mechanism and Simulation of Bi-Layered Micro Optical Fiber Resonator." Applied Mechanics and Materials 241-244 (December 2012): 841–46. http://dx.doi.org/10.4028/www.scientific.net/amm.241-244.841.

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Micro-resonators could be fabricated directly on the optical fiber top by micro mechanical process. The micro optical fiber resonator has more great advantages comparing with the traditional optical excited micro silicon resonators, such as being optically positioned easily between the resonator and the optical fiber end. By this way, the optical excited light through the fiber core is thus put on the micro resonator accurately and then partially reflected by the Fabry-Perot interferometer formed between fiber top and resonator surface. The reflected light from F-P interferometer was sent to t

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24

Gribovsky, A. V. "A FABRY-PEROT METARESONATOR SUPPORTING TRAPPED-MODE RESONANCES." Radio physics and radio astronomy 26, no. 4 (2021): 344–49. http://dx.doi.org/10.15407/rpra26.04.344.

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Purpose: Investigation of the electrodynamic properties of a Fabry-Perot metaresonator formed by two parallel perfectly conducting, two-dimensionally periodic, two-element screens of finite thickness with rectangular holes. The resonator is excited by a plane linearly polarized electromagnetic wave. The basic cell of each of the screens used as the metaresonator mirrors contains two lengths of rectangular waveguides of different transverse sections. Design/methodology/approach: An operator method for solving the 3D problems of electromagnetic wave diffraction by multielement two-dimensionally

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25

Wang, W., L. Zhang, K. Fang, and Y. W. Zhang. "Experimental study of EIT-Like phenomenon in a metamaterial plasma waveguide." Advanced Electromagnetics 1, no. 3 (2012): 61. http://dx.doi.org/10.7716/aem.v1i3.93.

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This paper demonstrates the realization of the electromagnetically induced transparency (EIT)-like transmission in a metamaterial plasma waveguide with double side defects based on transmission lines. The waveguide with a single side defect works as a plasma resonator and the resonance wavelength is determined by the Fabry-Perot resonance of surface plasma. While in a waveguide with double side defects, a transmission peak appears between the two resonators frequencies because of the destructive interference between the resonance modes of the two resonators, which indicates a pronounced EIT ph

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26

Britzger, Michael, Daniel Friedrich, Stefanie Kroker, et al. "Diffractively coupled Fabry-Perot resonator with power-recycling." Optics Express 19, no. 16 (2011): 14964. http://dx.doi.org/10.1364/oe.19.014964.

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27

Kollyukh, O. G. "Coherent thermal radiation of Fabry-Perot resonator structures." Semiconductor physics, quantum electronics and optoelectronics 10, no. 4 (2008): 94–102. http://dx.doi.org/10.15407/spqeo10.04.094.

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28

Pustovoit, V. I. "Acousto-optical analogue of a Fabry–Perot resonator." Quantum Electronics 51, no. 1 (2021): 73–78. http://dx.doi.org/10.1070/qel17399.

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29

Kagi, N., and K. Ema. "Optical pulse narrowing using a Fabry-Perot resonator." Applied Physics B Photophysics and Laser Chemistry 47, no. 4 (1988): 295–97. http://dx.doi.org/10.1007/bf00716088.

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30

Wu, Jiu Hui, Lay Kee Ang, Ai Qun Liu, Hwee Gee Teo, and Chao Lu. "Tunable high-Q photonic-bandgap Fabry-Perot resonator." Journal of the Optical Society of America B 22, no. 8 (2005): 1770. http://dx.doi.org/10.1364/josab.22.001770.

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31

Torchigin, V. P. "Waveguide analog of a nonlinear Fabry–Perot resonator." Soviet Journal of Quantum Electronics 22, no. 4 (1992): 357–61. http://dx.doi.org/10.1070/qe1992v022n04abeh003452.

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32

Belinskiĭ, A. V., and Anatolii S. Chirkin. "Fabry–Perot resonator with volume-distributed phase inhomogeneities." Soviet Journal of Quantum Electronics 16, no. 5 (1986): 685–87. http://dx.doi.org/10.1070/qe1986v016n05abeh006839.

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33

Поленга, С. В., Е. А. Литинская, А. В. Станковский та ін. "Антенная решетка Ku-диапазона частот на основе резонатора Фабри-Перо". Письма в журнал технической физики 49, № 13 (2023): 3. http://dx.doi.org/10.21883/pjtf.2023.13.55727.19550.

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The work is devoted to the development and study of the antenna array based on Fabry-Perot cavity in the radio band. The antenna array element in the form of a Fabry-Perot cavity with circular polarization is proposed, the semitransparent mirror of the cavity is realized in the form of a two-layer frequency-selective surface (FFS). A power divider based on thin waveguides to feed the antenna array with size 2x8 was developed. А model of the antenna array was manufactured. The power divider is made by laser cutting of sheet aluminum, semitransparent resonator layer is made by photolithography.

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34

Haindl, E., and K. Möbius. "A 94 GHz EPR Spectrometer with Fabry-Perot Resonator." Zeitschrift für Naturforschung A 40, no. 2 (1985): 169–72. http://dx.doi.org/10.1515/zna-1985-0211.

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An EPR spectrometer is described working in the 94 GHz (W-band) frequency range. It comprises a Fabry-Perot type microwave resonator connected to a conventional microwave bridge, a phase lock loop for microwave frequency stabilization, and a superconducting magnet. The improved separation of W-band spectra from two sites with only slightly different g-factors is demonstrated using an α-bromo radical in an X-irradiated 5-bromodeoxyuridine single crystal as example.

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35

Beneš, Jiří, František Procháska, Zdeněk Rail, David Tomka, Lenka Pravdová, and Ondřej Číp. "Production and measuring methods and procedures in precision optical cavities production." Journal of Instrumentation 17, no. 02 (2022): P02012. http://dx.doi.org/10.1088/1748-0221/17/02/p02012.

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Abstract This work presents the development of the production process of individual parts of the Fabry-Perot type laser resonator. It describes the acquired knowledge in the field of production of very precise optical standards, cavities, and lenses. In addition, it describes the measurement methods used in production. The work is intended for industry and science.

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36

Kaklamani, D. I. "Full-Wave Analysis of a Fabry-Perot Type Resonator." Progress In Electromagnetics Research 24 (1999): 279–310. http://dx.doi.org/10.2528/pier99042601.

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37

Ogusu, K., and S. Yamamoto. "Nonlinear fiber Fabry-Perot resonator using thermo-optic effect." Journal of Lightwave Technology 11, no. 11 (1993): 1774–81. http://dx.doi.org/10.1109/50.251174.

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38

Cox, A. J., and Dean C. Dibble. "Nondiffracting beam from a spatially filtered Fabry–Perot resonator." Journal of the Optical Society of America A 9, no. 2 (1992): 282. http://dx.doi.org/10.1364/josaa.9.000282.

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39

Gevorgyan, A. H., A. Zh Khachatryan, and N. M. Ispiryan. "Asymmetric Fabry-Perot resonator containing an arbitrary inhomogeneous layer." Technical Physics 48, no. 4 (2003): 460–68. http://dx.doi.org/10.1134/1.1568489.

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40

Pollnau, Markus. "Counter-propagating modes in a Fabry–Perot-type resonator." Optics Letters 43, no. 20 (2018): 5033. http://dx.doi.org/10.1364/ol.43.005033.

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41

Peerlings, J., A. Dehe, A. Vogt, et al. "Long resonator micromachined tunable GaAs-AlAs Fabry-Perot filter." IEEE Photonics Technology Letters 9, no. 9 (1997): 1235–37. http://dx.doi.org/10.1109/68.618489.

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42

Liptuga, Anatoliy, Vasyl Morozhenko, Viktor Pipa, Evgen Venger, and Theodor Kostiuk. "Faraday-active Fabry–Perot resonator: transmission, reflection, and emissivity." Journal of the Optical Society of America A 29, no. 5 (2012): 790. http://dx.doi.org/10.1364/josaa.29.000790.

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43

Klaassen, Thijs, Martin P. van Exter, and J. P. Woerdman. "Characterization of scattering in an optical Fabry-Perot resonator." Applied Optics 46, no. 22 (2007): 5210. http://dx.doi.org/10.1364/ao.46.005210.

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44

Kriegsmann, G. A. "Scattering matrix analysis of a photonic Fabry–Perot resonator." Wave Motion 37, no. 1 (2003): 43–61. http://dx.doi.org/10.1016/s0165-2125(02)00014-8.

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45

Zhao, Yan, Shu-Fang Fu, Hua Li, and Xuan-Zhang Wang. "Nonlinear Far-Infrared Transmission of Antiferromagnetic Fabry-Perot Resonator." IEEE Transactions on Magnetics 48, no. 4 (2012): 1597–600. http://dx.doi.org/10.1109/tmag.2011.2174350.

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46

Boutayeb, Halim, and Mourad Nedil. "High Gain Slot Array with Fabry-Perot Cavity Feeding Circuit." International Journal of Antennas and Propagation 2016 (2016): 1–5. http://dx.doi.org/10.1155/2016/9674742.

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A new approach for designing slot arrays using a Fabry-Perot cavity for the feeding circuit is presented. The proposed array has simpler and smaller feeding circuit compared to conventional feeding networks that have multiple dividers or combiners. The dividers and combiners are usually sources of losses. In addition, the profile of the proposed array is not limited by the half-wavelength resonance condition that exists for Fabry-Perot resonator antennas based on partially reflecting surfaces. The operating frequency is not sensitive to the profile of the antenna. A small profile can be achiev

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47

Kuvshinskii, Mickail, Sergei Oreshkin, Sergei Popov, et al. "Tests of Cryogenic Fabry–Perot Cavity with Mirrors on Different Substrates." Applied Sciences 9, no. 2 (2019): 230. http://dx.doi.org/10.3390/app9020230.

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Experiments were performed with Fabry–Perot optical resonators in vacuum at low temperatures. Mirrors were applied on substrates of various optical materials. An infrared laser with a wavelength of 1.064 microns was used. The pump power at the maximum could reach 450 mW. The evolution of the optical properties of the FP cavity was traced in the temperature range 300–10 K. The main parameters measured were the integral characteristics of the FP resonances–sharpness (finesse) and contrast of interference. Three types of substrates were tested: a sitall, an optical glass with ultra low thermal ex

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48

Wu, Y. H., Y. Y. Chang, Y. W. Tsai, and S. L. Chang. "Theoretical considerations in the construction of hard X-ray resonators at inclined incidence with ultra-high efficiency and resolution." Journal of Applied Crystallography 49, no. 5 (2016): 1653–58. http://dx.doi.org/10.1107/s1600576716012541.

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Detailed considerations of how to construct inclined-incidence hard X-ray resonators are presented. Owing to the symmetry of the crystals used, the Bragg back reflection usually employed in normal-incidence two- and multi-plate resonators to reflect the X-ray beam is often accompanied by unavoidable multiple-beam diffraction, and thus the reflectivity and cavity finesse are quite low. In contrast, crystal-based Fabry–Perot (FP) resonators at inclined incidence utilize multiple-beam diffraction to excite the back reflection inside the resonator to generate FP resonance with high efficiency, whi

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49

Kishioka, Kiyoshi, and Akihito Yamamoto. "An Analyzing Method of Series-Connected Fabry Perot Optical Resonator." IEEJ Transactions on Electronics, Information and Systems 125, no. 3 (2005): 530–31. http://dx.doi.org/10.1541/ieejeiss.125.530.

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50

Shi, Chao-Xiang. "Fabry–Perot resonator composed of a photoinduced birefringent fiber grating." Applied Optics 33, no. 30 (1994): 7002. http://dx.doi.org/10.1364/ao.33.007002.

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