Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF
Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda...
Ausführliche Beschreibung
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| Autor*in: |
Feng, Yongkang [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2023 |
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| Anmerkung: |
© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| Übergeordnetes Werk: |
Enthalten in: Optical and quantum electronics - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969, 55(2023), 4 vom: 17. Feb. |
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| Übergeordnetes Werk: |
volume:55 ; year:2023 ; number:4 ; day:17 ; month:02 |
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| DOI / URN: |
10.1007/s11082-023-04574-6 |
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| Katalog-ID: |
SPR049656902 |
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| 520 | |a Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. | ||
| 650 | 4 | |a Liquid-core photonic crystal fiber |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Finite element method |7 (dpeaa)DE-He213 | |
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| 650 | 4 | |a Nonlinearity |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Feng, Chun |4 aut | |
| 700 | 1 | |a Xu, Hongzhi |4 aut | |
| 700 | 1 | |a Jiang, Shubo |4 aut | |
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10.1007/s11082-023-04574-6 doi (DE-627)SPR049656902 (SPR)s11082-023-04574-6-e DE-627 ger DE-627 rakwb eng Feng, Yongkang verfasserin aut Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. Liquid-core photonic crystal fiber (dpeaa)DE-He213 Finite element method (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Nonlinearity (dpeaa)DE-He213 Feng, Chun aut Xu, Hongzhi aut Jiang, Shubo aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 55(2023), 4 vom: 17. Feb. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:55 year:2023 number:4 day:17 month:02 https://dx.doi.org/10.1007/s11082-023-04574-6 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_206 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_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_2119 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 55 2023 4 17 02 |
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10.1007/s11082-023-04574-6 doi (DE-627)SPR049656902 (SPR)s11082-023-04574-6-e DE-627 ger DE-627 rakwb eng Feng, Yongkang verfasserin aut Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. Liquid-core photonic crystal fiber (dpeaa)DE-He213 Finite element method (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Nonlinearity (dpeaa)DE-He213 Feng, Chun aut Xu, Hongzhi aut Jiang, Shubo aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 55(2023), 4 vom: 17. Feb. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:55 year:2023 number:4 day:17 month:02 https://dx.doi.org/10.1007/s11082-023-04574-6 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_206 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_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_2119 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 55 2023 4 17 02 |
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10.1007/s11082-023-04574-6 doi (DE-627)SPR049656902 (SPR)s11082-023-04574-6-e DE-627 ger DE-627 rakwb eng Feng, Yongkang verfasserin aut Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. Liquid-core photonic crystal fiber (dpeaa)DE-He213 Finite element method (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Nonlinearity (dpeaa)DE-He213 Feng, Chun aut Xu, Hongzhi aut Jiang, Shubo aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 55(2023), 4 vom: 17. Feb. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:55 year:2023 number:4 day:17 month:02 https://dx.doi.org/10.1007/s11082-023-04574-6 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_206 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_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_2119 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 55 2023 4 17 02 |
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10.1007/s11082-023-04574-6 doi (DE-627)SPR049656902 (SPR)s11082-023-04574-6-e DE-627 ger DE-627 rakwb eng Feng, Yongkang verfasserin aut Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. Liquid-core photonic crystal fiber (dpeaa)DE-He213 Finite element method (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Nonlinearity (dpeaa)DE-He213 Feng, Chun aut Xu, Hongzhi aut Jiang, Shubo aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 55(2023), 4 vom: 17. Feb. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:55 year:2023 number:4 day:17 month:02 https://dx.doi.org/10.1007/s11082-023-04574-6 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_206 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_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_2119 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 55 2023 4 17 02 |
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10.1007/s11082-023-04574-6 doi (DE-627)SPR049656902 (SPR)s11082-023-04574-6-e DE-627 ger DE-627 rakwb eng Feng, Yongkang verfasserin aut Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. Liquid-core photonic crystal fiber (dpeaa)DE-He213 Finite element method (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Nonlinearity (dpeaa)DE-He213 Feng, Chun aut Xu, Hongzhi aut Jiang, Shubo aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 55(2023), 4 vom: 17. Feb. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:55 year:2023 number:4 day:17 month:02 https://dx.doi.org/10.1007/s11082-023-04574-6 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_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 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_206 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_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_2119 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 55 2023 4 17 02 |
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Feng, Yongkang @@aut@@ Feng, Chun @@aut@@ Xu, Hongzhi @@aut@@ Jiang, Shubo @@aut@@ |
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Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. 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Feng, Yongkang |
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Feng, Yongkang misc Liquid-core photonic crystal fiber misc Finite element method misc Dispersion misc Nonlinearity Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF |
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Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF Liquid-core photonic crystal fiber (dpeaa)DE-He213 Finite element method (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Nonlinearity (dpeaa)DE-He213 |
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design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$cs_{2}%$ filled lcpcf |
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Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF |
| abstract |
Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstractGer |
Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstract_unstemmed |
Abstract Through filling CS%$_{2}%$ into the core, a liquid-core photonic crystal fiber(LCPCF) with a fully circular air hole structure was designed. The finite element method(FEM) and numerical analysis are combined to simulate the structure and optimize the parameters of the fiber. When %$\lambda =1550%$ nm ,the geometric optimal parameters are %$\Lambda =0.75\,\mu%$m, d%$_{1}/\Lambda =0.86%$, d%$_{2}/\Lambda =0.96%$, and d%$_{3}/\Lambda =0.20%$. Meanwhile, the LCPCF can achieve a large negative dispersion of %$-2697.06%$ ps/nm/km and a high nonlinearity of 50677.77 W%$^{-1}%$km%$^{-1}%$. The numerical aperture and light acceptance are 0.674 and 65.37%, respectively. By comparison, we believe that this LCPCF has obvious advantages in optical communication compensation and supercontinuum generation. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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4 |
| title_short |
Design and numerical analysis of large negative dispersion and ultra-high nonlinearity %$CS_{2}%$ filled LCPCF |
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https://dx.doi.org/10.1007/s11082-023-04574-6 |
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Feng, Chun Xu, Hongzhi Jiang, Shubo |
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Feng, Chun Xu, Hongzhi Jiang, Shubo |
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312693869 |
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| doi_str |
10.1007/s11082-023-04574-6 |
| up_date |
2024-07-04T01:44:36.459Z |
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1803610988437569536 |
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| score |
7.4011583 |