Fiber Optic Resonators for Angular Rate Sensors
Abstract Fiber-optic ring resonators can be used in various fields of science and technology as miniature sensors and sensors of physical quantities: an optoelectronic generator, a temperature and pressure sensor, biosensors, an angular rate sensor, etc. To determine the operating parameters of a me...
Ausführliche Beschreibung
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| Autor*in: |
Gilev, D. G. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2022 |
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| Anmerkung: |
© Allerton Press, Inc. 2022. ISSN 1062-8738, Bulletin of the Russian Academy of Sciences: Physics, 2022, Vol. 86, Suppl. 1, pp. S75–S80. © Allerton Press, Inc., 2022. |
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| Übergeordnetes Werk: |
Enthalten in: Bulletin of the Russian Academy of Sciences - New York, NY : Allerton Press, 2007, 86(2022), Suppl 1 vom: Dez., Seite S75-S80 |
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| Übergeordnetes Werk: |
volume:86 ; year:2022 ; number:Suppl 1 ; month:12 ; pages:S75-S80 |
| Links: |
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| DOI / URN: |
10.3103/S1062873822700423 |
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| Katalog-ID: |
SPR051329425 |
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| 520 | |a Abstract Fiber-optic ring resonators can be used in various fields of science and technology as miniature sensors and sensors of physical quantities: an optoelectronic generator, a temperature and pressure sensor, biosensors, an angular rate sensor, etc. To determine the operating parameters of a measuring sensor, it is necessary to measure the resonant parameters with an acceptable accuracy. These parameters are free spectral range (FSR), width at half maximum (FWHM), finesse (F) and quality factor (Q-factor).We have fabricated and investigated resonators, each of which is a closed fiber cavity of two fused couplers. The authors managed to reduce the error caused by the nonlinearity by using a reference asymmetric Mach–Zehnder interferometer and applying the Hilbert transforms. Synchronous measurement of the resonant spectrum and the beat signal coming from the interferometer during tuning of the laser center frequency and subsequent signal processing in a mathematical package made it possible to reduce the relative measurement error of the resonator performance parameters from 15 to 0.5%. This technique makes it possible to measure not only operating parameters with good accuracy, but also to record the change in these parameters, which improves the accuracy of detectors and sensors based on optical resonators. | ||
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| 700 | 1 | |a Chuvyzgalov, A. A. |0 (orcid)0000-0002-2017-9824 |4 aut | |
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10.3103/S1062873822700423 doi (DE-627)SPR051329425 (SPR)S1062873822700423-e DE-627 ger DE-627 rakwb eng Gilev, D. G. verfasserin (orcid)0000-0003-2589-7961 aut Fiber Optic Resonators for Angular Rate Sensors 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Allerton Press, Inc. 2022. ISSN 1062-8738, Bulletin of the Russian Academy of Sciences: Physics, 2022, Vol. 86, Suppl. 1, pp. S75–S80. © Allerton Press, Inc., 2022. Abstract Fiber-optic ring resonators can be used in various fields of science and technology as miniature sensors and sensors of physical quantities: an optoelectronic generator, a temperature and pressure sensor, biosensors, an angular rate sensor, etc. To determine the operating parameters of a measuring sensor, it is necessary to measure the resonant parameters with an acceptable accuracy. These parameters are free spectral range (FSR), width at half maximum (FWHM), finesse (F) and quality factor (Q-factor).We have fabricated and investigated resonators, each of which is a closed fiber cavity of two fused couplers. The authors managed to reduce the error caused by the nonlinearity by using a reference asymmetric Mach–Zehnder interferometer and applying the Hilbert transforms. Synchronous measurement of the resonant spectrum and the beat signal coming from the interferometer during tuning of the laser center frequency and subsequent signal processing in a mathematical package made it possible to reduce the relative measurement error of the resonator performance parameters from 15 to 0.5%. This technique makes it possible to measure not only operating parameters with good accuracy, but also to record the change in these parameters, which improves the accuracy of detectors and sensors based on optical resonators. Ovchinnikov, K. A. (orcid)0000-0001-9900-1799 aut Krishtop, V. V. (orcid)0000-0001-8871-8751 aut Chuvyzgalov, A. A. (orcid)0000-0002-2017-9824 aut Enthalten in Bulletin of the Russian Academy of Sciences New York, NY : Allerton Press, 2007 86(2022), Suppl 1 vom: Dez., Seite S75-S80 (DE-627)556723872 (DE-600)2403169-0 1934-9432 nnns volume:86 year:2022 number:Suppl 1 month:12 pages:S75-S80 https://dx.doi.org/10.3103/S1062873822700423 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 86 2022 Suppl 1 12 S75-S80 |
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10.3103/S1062873822700423 doi (DE-627)SPR051329425 (SPR)S1062873822700423-e DE-627 ger DE-627 rakwb eng Gilev, D. G. verfasserin (orcid)0000-0003-2589-7961 aut Fiber Optic Resonators for Angular Rate Sensors 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Allerton Press, Inc. 2022. ISSN 1062-8738, Bulletin of the Russian Academy of Sciences: Physics, 2022, Vol. 86, Suppl. 1, pp. S75–S80. © Allerton Press, Inc., 2022. Abstract Fiber-optic ring resonators can be used in various fields of science and technology as miniature sensors and sensors of physical quantities: an optoelectronic generator, a temperature and pressure sensor, biosensors, an angular rate sensor, etc. To determine the operating parameters of a measuring sensor, it is necessary to measure the resonant parameters with an acceptable accuracy. These parameters are free spectral range (FSR), width at half maximum (FWHM), finesse (F) and quality factor (Q-factor).We have fabricated and investigated resonators, each of which is a closed fiber cavity of two fused couplers. The authors managed to reduce the error caused by the nonlinearity by using a reference asymmetric Mach–Zehnder interferometer and applying the Hilbert transforms. Synchronous measurement of the resonant spectrum and the beat signal coming from the interferometer during tuning of the laser center frequency and subsequent signal processing in a mathematical package made it possible to reduce the relative measurement error of the resonator performance parameters from 15 to 0.5%. This technique makes it possible to measure not only operating parameters with good accuracy, but also to record the change in these parameters, which improves the accuracy of detectors and sensors based on optical resonators. Ovchinnikov, K. A. (orcid)0000-0001-9900-1799 aut Krishtop, V. V. (orcid)0000-0001-8871-8751 aut Chuvyzgalov, A. A. (orcid)0000-0002-2017-9824 aut Enthalten in Bulletin of the Russian Academy of Sciences New York, NY : Allerton Press, 2007 86(2022), Suppl 1 vom: Dez., Seite S75-S80 (DE-627)556723872 (DE-600)2403169-0 1934-9432 nnns volume:86 year:2022 number:Suppl 1 month:12 pages:S75-S80 https://dx.doi.org/10.3103/S1062873822700423 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 86 2022 Suppl 1 12 S75-S80 |
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10.3103/S1062873822700423 doi (DE-627)SPR051329425 (SPR)S1062873822700423-e DE-627 ger DE-627 rakwb eng Gilev, D. G. verfasserin (orcid)0000-0003-2589-7961 aut Fiber Optic Resonators for Angular Rate Sensors 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Allerton Press, Inc. 2022. ISSN 1062-8738, Bulletin of the Russian Academy of Sciences: Physics, 2022, Vol. 86, Suppl. 1, pp. S75–S80. © Allerton Press, Inc., 2022. Abstract Fiber-optic ring resonators can be used in various fields of science and technology as miniature sensors and sensors of physical quantities: an optoelectronic generator, a temperature and pressure sensor, biosensors, an angular rate sensor, etc. To determine the operating parameters of a measuring sensor, it is necessary to measure the resonant parameters with an acceptable accuracy. These parameters are free spectral range (FSR), width at half maximum (FWHM), finesse (F) and quality factor (Q-factor).We have fabricated and investigated resonators, each of which is a closed fiber cavity of two fused couplers. The authors managed to reduce the error caused by the nonlinearity by using a reference asymmetric Mach–Zehnder interferometer and applying the Hilbert transforms. Synchronous measurement of the resonant spectrum and the beat signal coming from the interferometer during tuning of the laser center frequency and subsequent signal processing in a mathematical package made it possible to reduce the relative measurement error of the resonator performance parameters from 15 to 0.5%. This technique makes it possible to measure not only operating parameters with good accuracy, but also to record the change in these parameters, which improves the accuracy of detectors and sensors based on optical resonators. Ovchinnikov, K. A. (orcid)0000-0001-9900-1799 aut Krishtop, V. V. (orcid)0000-0001-8871-8751 aut Chuvyzgalov, A. A. (orcid)0000-0002-2017-9824 aut Enthalten in Bulletin of the Russian Academy of Sciences New York, NY : Allerton Press, 2007 86(2022), Suppl 1 vom: Dez., Seite S75-S80 (DE-627)556723872 (DE-600)2403169-0 1934-9432 nnns volume:86 year:2022 number:Suppl 1 month:12 pages:S75-S80 https://dx.doi.org/10.3103/S1062873822700423 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 86 2022 Suppl 1 12 S75-S80 |
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Gilev, D. G. |
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| title_sort |
fiber optic resonators for angular rate sensors |
| title_auth |
Fiber Optic Resonators for Angular Rate Sensors |
| abstract |
Abstract Fiber-optic ring resonators can be used in various fields of science and technology as miniature sensors and sensors of physical quantities: an optoelectronic generator, a temperature and pressure sensor, biosensors, an angular rate sensor, etc. To determine the operating parameters of a measuring sensor, it is necessary to measure the resonant parameters with an acceptable accuracy. These parameters are free spectral range (FSR), width at half maximum (FWHM), finesse (F) and quality factor (Q-factor).We have fabricated and investigated resonators, each of which is a closed fiber cavity of two fused couplers. The authors managed to reduce the error caused by the nonlinearity by using a reference asymmetric Mach–Zehnder interferometer and applying the Hilbert transforms. Synchronous measurement of the resonant spectrum and the beat signal coming from the interferometer during tuning of the laser center frequency and subsequent signal processing in a mathematical package made it possible to reduce the relative measurement error of the resonator performance parameters from 15 to 0.5%. This technique makes it possible to measure not only operating parameters with good accuracy, but also to record the change in these parameters, which improves the accuracy of detectors and sensors based on optical resonators. © Allerton Press, Inc. 2022. ISSN 1062-8738, Bulletin of the Russian Academy of Sciences: Physics, 2022, Vol. 86, Suppl. 1, pp. S75–S80. © Allerton Press, Inc., 2022. |
| abstractGer |
Abstract Fiber-optic ring resonators can be used in various fields of science and technology as miniature sensors and sensors of physical quantities: an optoelectronic generator, a temperature and pressure sensor, biosensors, an angular rate sensor, etc. To determine the operating parameters of a measuring sensor, it is necessary to measure the resonant parameters with an acceptable accuracy. These parameters are free spectral range (FSR), width at half maximum (FWHM), finesse (F) and quality factor (Q-factor).We have fabricated and investigated resonators, each of which is a closed fiber cavity of two fused couplers. The authors managed to reduce the error caused by the nonlinearity by using a reference asymmetric Mach–Zehnder interferometer and applying the Hilbert transforms. Synchronous measurement of the resonant spectrum and the beat signal coming from the interferometer during tuning of the laser center frequency and subsequent signal processing in a mathematical package made it possible to reduce the relative measurement error of the resonator performance parameters from 15 to 0.5%. This technique makes it possible to measure not only operating parameters with good accuracy, but also to record the change in these parameters, which improves the accuracy of detectors and sensors based on optical resonators. © Allerton Press, Inc. 2022. ISSN 1062-8738, Bulletin of the Russian Academy of Sciences: Physics, 2022, Vol. 86, Suppl. 1, pp. S75–S80. © Allerton Press, Inc., 2022. |
| abstract_unstemmed |
Abstract Fiber-optic ring resonators can be used in various fields of science and technology as miniature sensors and sensors of physical quantities: an optoelectronic generator, a temperature and pressure sensor, biosensors, an angular rate sensor, etc. To determine the operating parameters of a measuring sensor, it is necessary to measure the resonant parameters with an acceptable accuracy. These parameters are free spectral range (FSR), width at half maximum (FWHM), finesse (F) and quality factor (Q-factor).We have fabricated and investigated resonators, each of which is a closed fiber cavity of two fused couplers. The authors managed to reduce the error caused by the nonlinearity by using a reference asymmetric Mach–Zehnder interferometer and applying the Hilbert transforms. Synchronous measurement of the resonant spectrum and the beat signal coming from the interferometer during tuning of the laser center frequency and subsequent signal processing in a mathematical package made it possible to reduce the relative measurement error of the resonator performance parameters from 15 to 0.5%. This technique makes it possible to measure not only operating parameters with good accuracy, but also to record the change in these parameters, which improves the accuracy of detectors and sensors based on optical resonators. © Allerton Press, Inc. 2022. ISSN 1062-8738, Bulletin of the Russian Academy of Sciences: Physics, 2022, Vol. 86, Suppl. 1, pp. S75–S80. © Allerton Press, Inc., 2022. |
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Fiber Optic Resonators for Angular Rate Sensors |
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Ovchinnikov, K. A. Krishtop, V. V. Chuvyzgalov, A. A. |
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