An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber
Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problem...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Khoobjou, Elham [verfasserIn] Khalesi, Hassan [verfasserIn] Ghods, Vahid [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2020 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Journal of electrical engineering & technology - [Singapore] : Springer Singapore, 2006, 15(2020), 6 vom: 27. Aug., Seite 2691-2698 |
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| Übergeordnetes Werk: |
volume:15 ; year:2020 ; number:6 ; day:27 ; month:08 ; pages:2691-2698 |
| Links: |
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| DOI / URN: |
10.1007/s42835-020-00526-2 |
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| Katalog-ID: |
SPR04173971X |
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| 245 | 1 | 3 | |a An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber |
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| 520 | |a Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). | ||
| 650 | 4 | |a Optical fiber |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Loss |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Dispersion |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Photonic crystal fiber (PCF) |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Germanium impurity |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Khalesi, Hassan |e verfasserin |4 aut | |
| 700 | 1 | |a Ghods, Vahid |e verfasserin |4 aut | |
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| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s42835-020-00526-2 |z lizenzpflichtig |3 Volltext |
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10.1007/s42835-020-00526-2 doi (DE-627)SPR04173971X (SPR)s42835-020-00526-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Khoobjou, Elham verfasserin aut An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). Optical fiber (dpeaa)DE-He213 Loss (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Photonic crystal fiber (PCF) (dpeaa)DE-He213 Germanium impurity (dpeaa)DE-He213 Khalesi, Hassan verfasserin aut Ghods, Vahid verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 15(2020), 6 vom: 27. Aug., Seite 2691-2698 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:15 year:2020 number:6 day:27 month:08 pages:2691-2698 https://dx.doi.org/10.1007/s42835-020-00526-2 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_105 GBV_ILN_110 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 15 2020 6 27 08 2691-2698 |
| spelling |
10.1007/s42835-020-00526-2 doi (DE-627)SPR04173971X (SPR)s42835-020-00526-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Khoobjou, Elham verfasserin aut An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). Optical fiber (dpeaa)DE-He213 Loss (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Photonic crystal fiber (PCF) (dpeaa)DE-He213 Germanium impurity (dpeaa)DE-He213 Khalesi, Hassan verfasserin aut Ghods, Vahid verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 15(2020), 6 vom: 27. Aug., Seite 2691-2698 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:15 year:2020 number:6 day:27 month:08 pages:2691-2698 https://dx.doi.org/10.1007/s42835-020-00526-2 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_105 GBV_ILN_110 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 15 2020 6 27 08 2691-2698 |
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10.1007/s42835-020-00526-2 doi (DE-627)SPR04173971X (SPR)s42835-020-00526-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Khoobjou, Elham verfasserin aut An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). Optical fiber (dpeaa)DE-He213 Loss (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Photonic crystal fiber (PCF) (dpeaa)DE-He213 Germanium impurity (dpeaa)DE-He213 Khalesi, Hassan verfasserin aut Ghods, Vahid verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 15(2020), 6 vom: 27. Aug., Seite 2691-2698 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:15 year:2020 number:6 day:27 month:08 pages:2691-2698 https://dx.doi.org/10.1007/s42835-020-00526-2 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_105 GBV_ILN_110 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 15 2020 6 27 08 2691-2698 |
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10.1007/s42835-020-00526-2 doi (DE-627)SPR04173971X (SPR)s42835-020-00526-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Khoobjou, Elham verfasserin aut An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). Optical fiber (dpeaa)DE-He213 Loss (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Photonic crystal fiber (PCF) (dpeaa)DE-He213 Germanium impurity (dpeaa)DE-He213 Khalesi, Hassan verfasserin aut Ghods, Vahid verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 15(2020), 6 vom: 27. Aug., Seite 2691-2698 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:15 year:2020 number:6 day:27 month:08 pages:2691-2698 https://dx.doi.org/10.1007/s42835-020-00526-2 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_105 GBV_ILN_110 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 15 2020 6 27 08 2691-2698 |
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10.1007/s42835-020-00526-2 doi (DE-627)SPR04173971X (SPR)s42835-020-00526-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Khoobjou, Elham verfasserin aut An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). Optical fiber (dpeaa)DE-He213 Loss (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Photonic crystal fiber (PCF) (dpeaa)DE-He213 Germanium impurity (dpeaa)DE-He213 Khalesi, Hassan verfasserin aut Ghods, Vahid verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 15(2020), 6 vom: 27. Aug., Seite 2691-2698 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:15 year:2020 number:6 day:27 month:08 pages:2691-2698 https://dx.doi.org/10.1007/s42835-020-00526-2 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_105 GBV_ILN_110 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 15 2020 6 27 08 2691-2698 |
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Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. 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Khoobjou, Elham |
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Khoobjou, Elham ddc 620 misc Optical fiber misc Loss misc Dispersion misc Photonic crystal fiber (PCF) misc Germanium impurity An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber |
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620 ASE An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber Optical fiber (dpeaa)DE-He213 Loss (dpeaa)DE-He213 Dispersion (dpeaa)DE-He213 Photonic crystal fiber (PCF) (dpeaa)DE-He213 Germanium impurity (dpeaa)DE-He213 |
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An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber |
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optimal design for decreasing dispersion in photonic crystal fiber |
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An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber |
| abstract |
Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). |
| abstractGer |
Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). |
| abstract_unstemmed |
Abstract Fiber optic transmission systems are friendly data transmission systems environmentally due to their low losses, high bandwidth and acceptable reliability. Therefore, they are often used for communication infrastructures. However, the effects of optical loss and dispersion can cause problems in fiber optic communications. In this paper, we mitigate these effects by using photonic crystals. The goal is to minimise the dispersion of the fibers by changing the photonic crystal fiber parameters. Specifically, we change the number, radius, and shape of the holes to minimise dispersion. A new photonic crystal fiber (PCF) is proposed with hexagonal grids of air holes and 11 layers in this structure. An optimal holes number, radius and distance between holes are used to obtain the least dispersion. Next, we use several elliptical and stellar holes to reduce dispersion. The germanium impurity is exploited in the PCF core as a defect. The addition of germanium impurity to the core causes the doping atoms reflect a stronger optical signal with the same attenuated input signal properties. The simulation results show that dispersion value is zero in three points at wavelengths between 1.48 and 1.55 μm. In this wavelength range, the dispersion value was obtained between − 0.3 and 0.6 ps/(nm km). |
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An Optimal Design for Decreasing Dispersion in Photonic Crystal Fiber |
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https://dx.doi.org/10.1007/s42835-020-00526-2 |
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Khalesi, Hassan Ghods, Vahid |
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Khalesi, Hassan Ghods, Vahid |
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| doi_str |
10.1007/s42835-020-00526-2 |
| up_date |
2024-07-03T23:27:36.751Z |
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