Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors
Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sen...
Ausführliche Beschreibung
Autor*in: |
Zaghloul, Seif eldin A. [verfasserIn] Yousif, Bedir [verfasserIn] Elzalabani, Mahmoud [verfasserIn] Areed, Nehal Fayez [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2017 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Optical and quantum electronics - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969, 49(2017), 11 vom: 07. Okt. |
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Übergeordnetes Werk: |
volume:49 ; year:2017 ; number:11 ; day:07 ; month:10 |
Links: |
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DOI / URN: |
10.1007/s11082-017-1180-7 |
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Katalog-ID: |
SPR016471946 |
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520 | |a Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. | ||
650 | 4 | |a Micro/nano fiber |7 (dpeaa)DE-He213 | |
650 | 4 | |a Leaky radiation |7 (dpeaa)DE-He213 | |
650 | 4 | |a Weaky radiation |7 (dpeaa)DE-He213 | |
650 | 4 | |a Petroleum productions |7 (dpeaa)DE-He213 | |
650 | 4 | |a Alcohols |7 (dpeaa)DE-He213 | |
700 | 1 | |a Yousif, Bedir |e verfasserin |4 aut | |
700 | 1 | |a Elzalabani, Mahmoud |e verfasserin |4 aut | |
700 | 1 | |a Areed, Nehal Fayez |e verfasserin |4 aut | |
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10.1007/s11082-017-1180-7 doi (DE-627)SPR016471946 (SPR)s11082-017-1180-7-e DE-627 ger DE-627 rakwb eng 500 620 ASE 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zaghloul, Seif eldin A. verfasserin aut Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. Micro/nano fiber (dpeaa)DE-He213 Leaky radiation (dpeaa)DE-He213 Weaky radiation (dpeaa)DE-He213 Petroleum productions (dpeaa)DE-He213 Alcohols (dpeaa)DE-He213 Yousif, Bedir verfasserin aut Elzalabani, Mahmoud verfasserin aut Areed, Nehal Fayez verfasserin aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 49(2017), 11 vom: 07. Okt. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:49 year:2017 number:11 day:07 month:10 https://dx.doi.org/10.1007/s11082-017-1180-7 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.38 ASE 33.18 ASE 33.23 ASE 53.54 ASE 52.88 ASE 33.72 ASE AR 49 2017 11 07 10 |
spelling |
10.1007/s11082-017-1180-7 doi (DE-627)SPR016471946 (SPR)s11082-017-1180-7-e DE-627 ger DE-627 rakwb eng 500 620 ASE 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zaghloul, Seif eldin A. verfasserin aut Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. Micro/nano fiber (dpeaa)DE-He213 Leaky radiation (dpeaa)DE-He213 Weaky radiation (dpeaa)DE-He213 Petroleum productions (dpeaa)DE-He213 Alcohols (dpeaa)DE-He213 Yousif, Bedir verfasserin aut Elzalabani, Mahmoud verfasserin aut Areed, Nehal Fayez verfasserin aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 49(2017), 11 vom: 07. Okt. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:49 year:2017 number:11 day:07 month:10 https://dx.doi.org/10.1007/s11082-017-1180-7 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.38 ASE 33.18 ASE 33.23 ASE 53.54 ASE 52.88 ASE 33.72 ASE AR 49 2017 11 07 10 |
allfields_unstemmed |
10.1007/s11082-017-1180-7 doi (DE-627)SPR016471946 (SPR)s11082-017-1180-7-e DE-627 ger DE-627 rakwb eng 500 620 ASE 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zaghloul, Seif eldin A. verfasserin aut Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. Micro/nano fiber (dpeaa)DE-He213 Leaky radiation (dpeaa)DE-He213 Weaky radiation (dpeaa)DE-He213 Petroleum productions (dpeaa)DE-He213 Alcohols (dpeaa)DE-He213 Yousif, Bedir verfasserin aut Elzalabani, Mahmoud verfasserin aut Areed, Nehal Fayez verfasserin aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 49(2017), 11 vom: 07. Okt. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:49 year:2017 number:11 day:07 month:10 https://dx.doi.org/10.1007/s11082-017-1180-7 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.38 ASE 33.18 ASE 33.23 ASE 53.54 ASE 52.88 ASE 33.72 ASE AR 49 2017 11 07 10 |
allfieldsGer |
10.1007/s11082-017-1180-7 doi (DE-627)SPR016471946 (SPR)s11082-017-1180-7-e DE-627 ger DE-627 rakwb eng 500 620 ASE 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zaghloul, Seif eldin A. verfasserin aut Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. Micro/nano fiber (dpeaa)DE-He213 Leaky radiation (dpeaa)DE-He213 Weaky radiation (dpeaa)DE-He213 Petroleum productions (dpeaa)DE-He213 Alcohols (dpeaa)DE-He213 Yousif, Bedir verfasserin aut Elzalabani, Mahmoud verfasserin aut Areed, Nehal Fayez verfasserin aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 49(2017), 11 vom: 07. Okt. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:49 year:2017 number:11 day:07 month:10 https://dx.doi.org/10.1007/s11082-017-1180-7 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.38 ASE 33.18 ASE 33.23 ASE 53.54 ASE 52.88 ASE 33.72 ASE AR 49 2017 11 07 10 |
allfieldsSound |
10.1007/s11082-017-1180-7 doi (DE-627)SPR016471946 (SPR)s11082-017-1180-7-e DE-627 ger DE-627 rakwb eng 500 620 ASE 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Zaghloul, Seif eldin A. verfasserin aut Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors 2017 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. Micro/nano fiber (dpeaa)DE-He213 Leaky radiation (dpeaa)DE-He213 Weaky radiation (dpeaa)DE-He213 Petroleum productions (dpeaa)DE-He213 Alcohols (dpeaa)DE-He213 Yousif, Bedir verfasserin aut Elzalabani, Mahmoud verfasserin aut Areed, Nehal Fayez verfasserin aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 49(2017), 11 vom: 07. Okt. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:49 year:2017 number:11 day:07 month:10 https://dx.doi.org/10.1007/s11082-017-1180-7 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_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 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_2116 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_4012 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_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.38 ASE 33.18 ASE 33.23 ASE 53.54 ASE 52.88 ASE 33.72 ASE AR 49 2017 11 07 10 |
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English |
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Enthalten in Optical and quantum electronics 49(2017), 11 vom: 07. Okt. volume:49 year:2017 number:11 day:07 month:10 |
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Enthalten in Optical and quantum electronics 49(2017), 11 vom: 07. Okt. volume:49 year:2017 number:11 day:07 month:10 |
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Micro/nano fiber Leaky radiation Weaky radiation Petroleum productions Alcohols |
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Optical and quantum electronics |
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Zaghloul, Seif eldin A. @@aut@@ Yousif, Bedir @@aut@@ Elzalabani, Mahmoud @@aut@@ Areed, Nehal Fayez @@aut@@ |
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2017-10-07T00:00:00Z |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR016471946</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111032202.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2017 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11082-017-1180-7</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR016471946</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s11082-017-1180-7-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">500</subfield><subfield code="a">620</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.38</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.18</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.23</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">53.54</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">52.88</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.72</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Zaghloul, Seif eldin A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2017</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. 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|
author |
Zaghloul, Seif eldin A. |
spellingShingle |
Zaghloul, Seif eldin A. ddc 500 bkl 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 misc Micro/nano fiber misc Leaky radiation misc Weaky radiation misc Petroleum productions misc Alcohols Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
authorStr |
Zaghloul, Seif eldin A. |
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@@773@@(DE-627)312693869 |
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electronic Article |
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500 - Natural sciences & mathematics 620 - Engineering & allied operations |
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aut aut aut aut |
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springer |
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true |
illustrated |
Not Illustrated |
issn |
1572-817X |
topic_title |
500 620 ASE 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors Micro/nano fiber (dpeaa)DE-He213 Leaky radiation (dpeaa)DE-He213 Weaky radiation (dpeaa)DE-He213 Petroleum productions (dpeaa)DE-He213 Alcohols (dpeaa)DE-He213 |
topic |
ddc 500 bkl 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 misc Micro/nano fiber misc Leaky radiation misc Weaky radiation misc Petroleum productions misc Alcohols |
topic_unstemmed |
ddc 500 bkl 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 misc Micro/nano fiber misc Leaky radiation misc Weaky radiation misc Petroleum productions misc Alcohols |
topic_browse |
ddc 500 bkl 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 misc Micro/nano fiber misc Leaky radiation misc Weaky radiation misc Petroleum productions misc Alcohols |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Optical and quantum electronics |
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Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
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Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
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Zaghloul, Seif eldin A. |
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Optical and quantum electronics |
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Zaghloul, Seif eldin A. Yousif, Bedir Elzalabani, Mahmoud Areed, Nehal Fayez |
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Elektronische Aufsätze |
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Zaghloul, Seif eldin A. |
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sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
title_auth |
Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
abstract |
Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. |
abstractGer |
Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. |
abstract_unstemmed |
Abstract The maximization of sensitivities of both leaky and weakly radiation micro/nano fiber sensors based on the refractive index occurred by choose the suitable core material ($ n_{f} $) for each environmental material ($ n_{e} $) with a specific wavelength ($ λ_{max} $) at which the highest sensitivity is achieved. Where the refractive indices $ n_{f} $ and $ n_{e} $ are wavelength dependent. For the leaky radiation microfiber sensor, the value of $ n_{f} $ less than and getting close to the value of $ n_{e} $. The core material can be available with environmental material at some wavelengths and not suitable with other wavelengths. Such as, the core (BK7 glass) unsuitable with styrene within band rejected wavelengths (λ = 0.783–1.033) from the transmittance range of styrene (λ = 0.4386–1.052 μm). The radiation angle sensitivity ($ S_{θ} $) becomes very high with wavelength ($ λ_{Sθmax} $) at which $ n_{f} $ ≈ $ n_{e} $. Such as, core (BK7 glass) and environmental (styrene) at $ λ_{max} $ = 0.8 μm, the value of $ S_{θ} $ = 13759. In the weakly radiation, the value of $ n_{f} $ greater than the value of $ n_{e} $. The sensitivity is evaluated by measurement the mode field radius ($ S_{W} $) or the fiber core power ($ S_{P} $). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity $ S_{w} $ = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity $ S_{P} $ = 22.3 $ P_{i} $ (power unit/RIU) at λ = 1.05 μm ($ P_{i} $ is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity ($ S_{θ} $) are excellent if they are compared with the published experimental measured results. The leaky and weakly sensors has potential applications due to their high sensitivity and simple constructions. |
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title_short |
Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
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https://dx.doi.org/10.1007/s11082-017-1180-7 |
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|
score |
7.4009256 |