Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator

Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies wi...
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Autor*in:	Quanjing Zhao [verfasserIn] Juanjuan Yan [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Schlagwörter:	dual‐parallel Mach–Zehnder modulator optoelectronic oscillator tri‐band frequencies

Übergeordnetes Werk:	In: IET Optoelectronics - Wiley, 2021, 16(2022), 5, Seite 218-224
Übergeordnetes Werk:	volume:16 ; year:2022 ; number:5 ; pages:218-224

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc Journal toc

DOI / URN:	10.1049/ote2.12075

Katalog-ID:	DOAJ034129847

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520			\|a Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively.
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publishDate	2022
allfields	10.1049/ote2.12075 doi (DE-627)DOAJ034129847 (DE-599)DOAJ484ff157689540bd90aa32871113f96d DE-627 ger DE-627 rakwb eng TA1501-1820 Quanjing Zhao verfasserin aut Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively. dual‐parallel Mach–Zehnder modulator optoelectronic oscillator tri‐band frequencies Applied optics. Photonics Juanjuan Yan verfasserin aut In IET Optoelectronics Wiley, 2021 16(2022), 5, Seite 218-224 (DE-627)521693683 (DE-600)2264530-5 17518776 nnns volume:16 year:2022 number:5 pages:218-224 https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/article/484ff157689540bd90aa32871113f96d kostenfrei https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/toc/1751-8768 Journal toc kostenfrei https://doaj.org/toc/1751-8776 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 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_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 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_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 16 2022 5 218-224
spelling	10.1049/ote2.12075 doi (DE-627)DOAJ034129847 (DE-599)DOAJ484ff157689540bd90aa32871113f96d DE-627 ger DE-627 rakwb eng TA1501-1820 Quanjing Zhao verfasserin aut Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively. dual‐parallel Mach–Zehnder modulator optoelectronic oscillator tri‐band frequencies Applied optics. Photonics Juanjuan Yan verfasserin aut In IET Optoelectronics Wiley, 2021 16(2022), 5, Seite 218-224 (DE-627)521693683 (DE-600)2264530-5 17518776 nnns volume:16 year:2022 number:5 pages:218-224 https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/article/484ff157689540bd90aa32871113f96d kostenfrei https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/toc/1751-8768 Journal toc kostenfrei https://doaj.org/toc/1751-8776 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 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_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 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_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 16 2022 5 218-224
allfields_unstemmed	10.1049/ote2.12075 doi (DE-627)DOAJ034129847 (DE-599)DOAJ484ff157689540bd90aa32871113f96d DE-627 ger DE-627 rakwb eng TA1501-1820 Quanjing Zhao verfasserin aut Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively. dual‐parallel Mach–Zehnder modulator optoelectronic oscillator tri‐band frequencies Applied optics. Photonics Juanjuan Yan verfasserin aut In IET Optoelectronics Wiley, 2021 16(2022), 5, Seite 218-224 (DE-627)521693683 (DE-600)2264530-5 17518776 nnns volume:16 year:2022 number:5 pages:218-224 https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/article/484ff157689540bd90aa32871113f96d kostenfrei https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/toc/1751-8768 Journal toc kostenfrei https://doaj.org/toc/1751-8776 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 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_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 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_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 16 2022 5 218-224
allfieldsGer	10.1049/ote2.12075 doi (DE-627)DOAJ034129847 (DE-599)DOAJ484ff157689540bd90aa32871113f96d DE-627 ger DE-627 rakwb eng TA1501-1820 Quanjing Zhao verfasserin aut Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively. dual‐parallel Mach–Zehnder modulator optoelectronic oscillator tri‐band frequencies Applied optics. Photonics Juanjuan Yan verfasserin aut In IET Optoelectronics Wiley, 2021 16(2022), 5, Seite 218-224 (DE-627)521693683 (DE-600)2264530-5 17518776 nnns volume:16 year:2022 number:5 pages:218-224 https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/article/484ff157689540bd90aa32871113f96d kostenfrei https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/toc/1751-8768 Journal toc kostenfrei https://doaj.org/toc/1751-8776 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 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_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 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_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 16 2022 5 218-224
allfieldsSound	10.1049/ote2.12075 doi (DE-627)DOAJ034129847 (DE-599)DOAJ484ff157689540bd90aa32871113f96d DE-627 ger DE-627 rakwb eng TA1501-1820 Quanjing Zhao verfasserin aut Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively. dual‐parallel Mach–Zehnder modulator optoelectronic oscillator tri‐band frequencies Applied optics. Photonics Juanjuan Yan verfasserin aut In IET Optoelectronics Wiley, 2021 16(2022), 5, Seite 218-224 (DE-627)521693683 (DE-600)2264530-5 17518776 nnns volume:16 year:2022 number:5 pages:218-224 https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/article/484ff157689540bd90aa32871113f96d kostenfrei https://doi.org/10.1049/ote2.12075 kostenfrei https://doaj.org/toc/1751-8768 Journal toc kostenfrei https://doaj.org/toc/1751-8776 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 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_2034 GBV_ILN_2037 GBV_ILN_2038 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_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 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_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2470 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 AR 16 2022 5 218-224
language	English
source	In IET Optoelectronics 16(2022), 5, Seite 218-224 volume:16 year:2022 number:5 pages:218-224
sourceStr	In IET Optoelectronics 16(2022), 5, Seite 218-224 volume:16 year:2022 number:5 pages:218-224
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	dual‐parallel Mach–Zehnder modulator optoelectronic oscillator tri‐band frequencies Applied optics. Photonics
isfreeaccess_bool	true
container_title	IET Optoelectronics
authorswithroles_txt_mv	Quanjing Zhao @@aut@@ Juanjuan Yan @@aut@@
publishDateDaySort_date	2022-01-01T00:00:00Z
hierarchy_top_id	521693683
id	DOAJ034129847
language_de	englisch
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callnumber-first	T - Technology
author	Quanjing Zhao
spellingShingle	Quanjing Zhao misc TA1501-1820 misc dual‐parallel Mach–Zehnder modulator misc optoelectronic oscillator misc tri‐band frequencies misc Applied optics. Photonics Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator
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topic_title	TA1501-1820 Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator dual‐parallel Mach–Zehnder modulator optoelectronic oscillator tri‐band frequencies
topic	misc TA1501-1820 misc dual‐parallel Mach–Zehnder modulator misc optoelectronic oscillator misc tri‐band frequencies misc Applied optics. Photonics
topic_unstemmed	misc TA1501-1820 misc dual‐parallel Mach–Zehnder modulator misc optoelectronic oscillator misc tri‐band frequencies misc Applied optics. Photonics
topic_browse	misc TA1501-1820 misc dual‐parallel Mach–Zehnder modulator misc optoelectronic oscillator misc tri‐band frequencies misc Applied optics. Photonics
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title	Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator
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title_full	Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator
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title_sort	self‐starting generation of tri‐band frequencies using a dual‐parallel mach–zehnder modulator‐based optoelectronic oscillator
callnumber	TA1501-1820
title_auth	Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator
abstract	Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively.
abstractGer	Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively.
abstract_unstemmed	Abstract A scheme for multi‐band frequency generation is proposed and experimentally demonstrated using a dual‐parallel Mach–Zehnder modulator (DPMZM)‐based optoelectronic oscillator (OEO). The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively.
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title_short	Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator
url	https://doi.org/10.1049/ote2.12075 https://doaj.org/article/484ff157689540bd90aa32871113f96d https://doaj.org/toc/1751-8768 https://doaj.org/toc/1751-8776
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doi_str	10.1049/ote2.12075
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up_date	2024-07-03T21:35:15.628Z
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The principle of this generator is theoretically described in detail. It is found that multiple frequencies with a small power variation can be produced by setting the three working points and the modulation depth of the DPMZM. In the proving experiment, an 8‐GHz fundamental oscillation with a side mode suppression ratio of 44 dB is generated. The phase noise is measured to be −96.8 dBc/Hz 10 KHz offset with a 100‐m and 1‐Km optical fibre used in the two oscillation loops. When the oscillating signal is applied to drive the two sub‐modulators in the DPMZM, doubled and tripled frequencies are produced at the same time, and the phase noises of the two frequencies are also measured to be −90.2 dBc/Hz and −85.9 dBc/Hz @10 KHz, respectively.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">dual‐parallel Mach–Zehnder modulator</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">optoelectronic oscillator</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">tri‐band frequencies</subfield></datafield><datafield tag="653" ind1=" " ind2="0"><subfield code="a">Applied optics. Photonics</subfield></datafield><datafield tag="700" ind1="0" ind2=" "><subfield code="a">Juanjuan Yan</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">In</subfield><subfield code="t">IET Optoelectronics</subfield><subfield code="d">Wiley, 2021</subfield><subfield code="g">16(2022), 5, Seite 218-224</subfield><subfield code="w">(DE-627)521693683</subfield><subfield code="w">(DE-600)2264530-5</subfield><subfield code="x">17518776</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:16</subfield><subfield code="g">year:2022</subfield><subfield code="g">number:5</subfield><subfield code="g">pages:218-224</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.1049/ote2.12075</subfield><subfield code="z">kostenfrei</subfield></datafield><datafield tag="856" ind1="4" 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Self‐starting generation of tri‐band frequencies using a dual‐parallel Mach–Zehnder modulator‐based optoelectronic oscillator

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