Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors
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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where th...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Zaghloul, Seif eldin A [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2017 |
|---|
| Rechteinformationen: |
Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017 |
|---|
| Schlagwörter: |
Computer Communication Networks Optics, Lasers, Photonics, Optical Devices |
|---|
| Übergeordnetes Werk: |
Enthalten in: Optical and quantum electronics - Dordrecht : Kluwer, 1975, 49(2017), 11, Seite 1-21 |
|---|---|
| Übergeordnetes Werk: |
volume:49 ; year:2017 ; number:11 ; pages:1-21 |
| Links: |
|---|
| DOI / URN: |
10.1007/s11082-017-1180-7 |
|---|
| Katalog-ID: |
OLC1996850040 |
|---|
| LEADER | 01000caa a2200265 4500 | ||
|---|---|---|---|
| 001 | OLC1996850040 | ||
| 003 | DE-627 | ||
| 005 | 20220219202958.0 | ||
| 007 | tu | ||
| 008 | 171125s2017 xx ||||| 00| ||eng c | ||
| 024 | 7 | |a 10.1007/s11082-017-1180-7 |2 doi | |
| 028 | 5 | 2 | |a PQ20171228 |
| 035 | |a (DE-627)OLC1996850040 | ||
| 035 | |a (DE-599)GBVOLC1996850040 | ||
| 035 | |a (PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590 | ||
| 035 | |a (KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic | ||
| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 082 | 0 | 4 | |a 500 |a 620 |q DE-600 |
| 084 | |a 33.38 |2 bkl | ||
| 084 | |a 33.18 |2 bkl | ||
| 084 | |a 33.23 |2 bkl | ||
| 084 | |a 53.54 |2 bkl | ||
| 084 | |a 52.88 |2 bkl | ||
| 084 | |a 33.72 |2 bkl | ||
| 100 | 1 | |a Zaghloul, Seif eldin A |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
| 264 | 1 | |c 2017 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a ohne Hilfsmittel zu benutzen |b n |2 rdamedia | ||
| 338 | |a Band |b nc |2 rdacarrier | ||
| 520 | |a 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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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. | ||
| 540 | |a Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017 | ||
| 650 | 4 | |a Leaky radiation | |
| 650 | 4 | |a Physics | |
| 650 | 4 | |a Computer Communication Networks | |
| 650 | 4 | |a Alcohols | |
| 650 | 4 | |a Electrical Engineering | |
| 650 | 4 | |a Petroleum productions | |
| 650 | 4 | |a Micro/nano fiber | |
| 650 | 4 | |a Optics, Lasers, Photonics, Optical Devices | |
| 650 | 4 | |a Weaky radiation | |
| 650 | 4 | |a Characterization and Evaluation of Materials | |
| 650 | 4 | |a Sensors | |
| 650 | 4 | |a Sensitivity analysis | |
| 650 | 4 | |a Toluene | |
| 650 | 4 | |a Refractivity | |
| 650 | 4 | |a Maximization | |
| 650 | 4 | |a Wavelengths | |
| 700 | 1 | |a Yousif, Bedir |4 oth | |
| 700 | 1 | |a Elzalabani, Mahmoud |4 oth | |
| 700 | 1 | |a Areed, Nehal Fayez |4 oth | |
| 773 | 0 | 8 | |i Enthalten in |t Optical and quantum electronics |d Dordrecht : Kluwer, 1975 |g 49(2017), 11, Seite 1-21 |w (DE-627)129419540 |w (DE-600)189950-8 |w (DE-576)014796139 |x 0306-8919 |7 nnns |
| 773 | 1 | 8 | |g volume:49 |g year:2017 |g number:11 |g pages:1-21 |
| 856 | 4 | 1 | |u http://dx.doi.org/10.1007/s11082-017-1180-7 |3 Volltext |
| 856 | 4 | 2 | |u https://search.proquest.com/docview/1948153330 |
| 912 | |a GBV_USEFLAG_A | ||
| 912 | |a SYSFLAG_A | ||
| 912 | |a GBV_OLC | ||
| 912 | |a SSG-OLC-TEC | ||
| 912 | |a SSG-OLC-PHY | ||
| 912 | |a GBV_ILN_22 | ||
| 912 | |a GBV_ILN_70 | ||
| 912 | |a GBV_ILN_150 | ||
| 936 | b | k | |a 33.38 |q AVZ |
| 936 | b | k | |a 33.18 |q AVZ |
| 936 | b | k | |a 33.23 |q AVZ |
| 936 | b | k | |a 53.54 |q AVZ |
| 936 | b | k | |a 52.88 |q AVZ |
| 936 | b | k | |a 33.72 |q AVZ |
| 951 | |a AR | ||
| 952 | |d 49 |j 2017 |e 11 |h 1-21 | ||
| author_variant |
s e a z sea seaz |
|---|---|
| matchkey_str |
article:03068919:2017----::estvtmxmztoolaynwayaitomc |
| hierarchy_sort_str |
2017 |
| bklnumber |
33.38 33.18 33.23 53.54 52.88 33.72 |
| publishDate |
2017 |
| allfields |
10.1007/s11082-017-1180-7 doi PQ20171228 (DE-627)OLC1996850040 (DE-599)GBVOLC1996850040 (PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590 (KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic DE-627 ger DE-627 rakwb eng 500 620 DE-600 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 ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier 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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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. Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017 Leaky radiation Physics Computer Communication Networks Alcohols Electrical Engineering Petroleum productions Micro/nano fiber Optics, Lasers, Photonics, Optical Devices Weaky radiation Characterization and Evaluation of Materials Sensors Sensitivity analysis Toluene Refractivity Maximization Wavelengths Yousif, Bedir oth Elzalabani, Mahmoud oth Areed, Nehal Fayez oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 49(2017), 11, Seite 1-21 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:49 year:2017 number:11 pages:1-21 http://dx.doi.org/10.1007/s11082-017-1180-7 Volltext https://search.proquest.com/docview/1948153330 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 49 2017 11 1-21 |
| spelling |
10.1007/s11082-017-1180-7 doi PQ20171228 (DE-627)OLC1996850040 (DE-599)GBVOLC1996850040 (PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590 (KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic DE-627 ger DE-627 rakwb eng 500 620 DE-600 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 ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier 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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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. Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017 Leaky radiation Physics Computer Communication Networks Alcohols Electrical Engineering Petroleum productions Micro/nano fiber Optics, Lasers, Photonics, Optical Devices Weaky radiation Characterization and Evaluation of Materials Sensors Sensitivity analysis Toluene Refractivity Maximization Wavelengths Yousif, Bedir oth Elzalabani, Mahmoud oth Areed, Nehal Fayez oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 49(2017), 11, Seite 1-21 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:49 year:2017 number:11 pages:1-21 http://dx.doi.org/10.1007/s11082-017-1180-7 Volltext https://search.proquest.com/docview/1948153330 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 49 2017 11 1-21 |
| allfields_unstemmed |
10.1007/s11082-017-1180-7 doi PQ20171228 (DE-627)OLC1996850040 (DE-599)GBVOLC1996850040 (PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590 (KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic DE-627 ger DE-627 rakwb eng 500 620 DE-600 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 ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier 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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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. Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017 Leaky radiation Physics Computer Communication Networks Alcohols Electrical Engineering Petroleum productions Micro/nano fiber Optics, Lasers, Photonics, Optical Devices Weaky radiation Characterization and Evaluation of Materials Sensors Sensitivity analysis Toluene Refractivity Maximization Wavelengths Yousif, Bedir oth Elzalabani, Mahmoud oth Areed, Nehal Fayez oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 49(2017), 11, Seite 1-21 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:49 year:2017 number:11 pages:1-21 http://dx.doi.org/10.1007/s11082-017-1180-7 Volltext https://search.proquest.com/docview/1948153330 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 49 2017 11 1-21 |
| allfieldsGer |
10.1007/s11082-017-1180-7 doi PQ20171228 (DE-627)OLC1996850040 (DE-599)GBVOLC1996850040 (PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590 (KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic DE-627 ger DE-627 rakwb eng 500 620 DE-600 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 ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier 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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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. Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017 Leaky radiation Physics Computer Communication Networks Alcohols Electrical Engineering Petroleum productions Micro/nano fiber Optics, Lasers, Photonics, Optical Devices Weaky radiation Characterization and Evaluation of Materials Sensors Sensitivity analysis Toluene Refractivity Maximization Wavelengths Yousif, Bedir oth Elzalabani, Mahmoud oth Areed, Nehal Fayez oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 49(2017), 11, Seite 1-21 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:49 year:2017 number:11 pages:1-21 http://dx.doi.org/10.1007/s11082-017-1180-7 Volltext https://search.proquest.com/docview/1948153330 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 49 2017 11 1-21 |
| allfieldsSound |
10.1007/s11082-017-1180-7 doi PQ20171228 (DE-627)OLC1996850040 (DE-599)GBVOLC1996850040 (PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590 (KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic DE-627 ger DE-627 rakwb eng 500 620 DE-600 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 ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier 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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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. Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017 Leaky radiation Physics Computer Communication Networks Alcohols Electrical Engineering Petroleum productions Micro/nano fiber Optics, Lasers, Photonics, Optical Devices Weaky radiation Characterization and Evaluation of Materials Sensors Sensitivity analysis Toluene Refractivity Maximization Wavelengths Yousif, Bedir oth Elzalabani, Mahmoud oth Areed, Nehal Fayez oth Enthalten in Optical and quantum electronics Dordrecht : Kluwer, 1975 49(2017), 11, Seite 1-21 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:49 year:2017 number:11 pages:1-21 http://dx.doi.org/10.1007/s11082-017-1180-7 Volltext https://search.proquest.com/docview/1948153330 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 33.38 AVZ 33.18 AVZ 33.23 AVZ 53.54 AVZ 52.88 AVZ 33.72 AVZ AR 49 2017 11 1-21 |
| language |
English |
| source |
Enthalten in Optical and quantum electronics 49(2017), 11, Seite 1-21 volume:49 year:2017 number:11 pages:1-21 |
| sourceStr |
Enthalten in Optical and quantum electronics 49(2017), 11, Seite 1-21 volume:49 year:2017 number:11 pages:1-21 |
| format_phy_str_mv |
Article |
| institution |
findex.gbv.de |
| topic_facet |
Leaky radiation Physics Computer Communication Networks Alcohols Electrical Engineering Petroleum productions Micro/nano fiber Optics, Lasers, Photonics, Optical Devices Weaky radiation Characterization and Evaluation of Materials Sensors Sensitivity analysis Toluene Refractivity Maximization Wavelengths |
| dewey-raw |
500 |
| isfreeaccess_bool |
false |
| container_title |
Optical and quantum electronics |
| authorswithroles_txt_mv |
Zaghloul, Seif eldin A @@aut@@ Yousif, Bedir @@oth@@ Elzalabani, Mahmoud @@oth@@ Areed, Nehal Fayez @@oth@@ |
| publishDateDaySort_date |
2017-01-01T00:00:00Z |
| hierarchy_top_id |
129419540 |
| dewey-sort |
3500 |
| id |
OLC1996850040 |
| language_de |
englisch |
| fullrecord |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a2200265 4500</leader><controlfield tag="001">OLC1996850040</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220219202958.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">171125s2017 xx ||||| 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="028" ind1="5" ind2="2"><subfield code="a">PQ20171228</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC1996850040</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVOLC1996850040</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic</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">DE-600</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">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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.</subfield></datafield><datafield tag="540" ind1=" " ind2=" "><subfield code="a">Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Leaky radiation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Physics</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Computer Communication Networks</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Alcohols</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Electrical Engineering</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Petroleum productions</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Micro/nano fiber</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Optics, Lasers, Photonics, Optical Devices</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Weaky radiation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Characterization and Evaluation of Materials</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Sensors</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Sensitivity analysis</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Toluene</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Refractivity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Maximization</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Wavelengths</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Yousif, Bedir</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Elzalabani, Mahmoud</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Areed, Nehal Fayez</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Optical and quantum electronics</subfield><subfield code="d">Dordrecht : Kluwer, 1975</subfield><subfield code="g">49(2017), 11, Seite 1-21</subfield><subfield code="w">(DE-627)129419540</subfield><subfield code="w">(DE-600)189950-8</subfield><subfield code="w">(DE-576)014796139</subfield><subfield code="x">0306-8919</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:49</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:11</subfield><subfield code="g">pages:1-21</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">http://dx.doi.org/10.1007/s11082-017-1180-7</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://search.proquest.com/docview/1948153330</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_150</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.38</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.18</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.23</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">53.54</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">52.88</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.72</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">49</subfield><subfield code="j">2017</subfield><subfield code="e">11</subfield><subfield code="h">1-21</subfield></datafield></record></collection>
|
| 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 Leaky radiation misc Physics misc Computer Communication Networks misc Alcohols misc Electrical Engineering misc Petroleum productions misc Micro/nano fiber misc Optics, Lasers, Photonics, Optical Devices misc Weaky radiation misc Characterization and Evaluation of Materials misc Sensors misc Sensitivity analysis misc Toluene misc Refractivity misc Maximization misc Wavelengths Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
| authorStr |
Zaghloul, Seif eldin A |
| ppnlink_with_tag_str_mv |
@@773@@(DE-627)129419540 |
| format |
Article |
| dewey-ones |
500 - Natural sciences & mathematics 620 - Engineering & allied operations |
| delete_txt_mv |
keep |
| author_role |
aut |
| collection |
OLC |
| remote_str |
false |
| illustrated |
Not Illustrated |
| issn |
0306-8919 |
| topic_title |
500 620 DE-600 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 Leaky radiation Physics Computer Communication Networks Alcohols Electrical Engineering Petroleum productions Micro/nano fiber Optics, Lasers, Photonics, Optical Devices Weaky radiation Characterization and Evaluation of Materials Sensors Sensitivity analysis Toluene Refractivity Maximization Wavelengths |
| topic |
ddc 500 bkl 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 misc Leaky radiation misc Physics misc Computer Communication Networks misc Alcohols misc Electrical Engineering misc Petroleum productions misc Micro/nano fiber misc Optics, Lasers, Photonics, Optical Devices misc Weaky radiation misc Characterization and Evaluation of Materials misc Sensors misc Sensitivity analysis misc Toluene misc Refractivity misc Maximization misc Wavelengths |
| topic_unstemmed |
ddc 500 bkl 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 misc Leaky radiation misc Physics misc Computer Communication Networks misc Alcohols misc Electrical Engineering misc Petroleum productions misc Micro/nano fiber misc Optics, Lasers, Photonics, Optical Devices misc Weaky radiation misc Characterization and Evaluation of Materials misc Sensors misc Sensitivity analysis misc Toluene misc Refractivity misc Maximization misc Wavelengths |
| topic_browse |
ddc 500 bkl 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 misc Leaky radiation misc Physics misc Computer Communication Networks misc Alcohols misc Electrical Engineering misc Petroleum productions misc Micro/nano fiber misc Optics, Lasers, Photonics, Optical Devices misc Weaky radiation misc Characterization and Evaluation of Materials misc Sensors misc Sensitivity analysis misc Toluene misc Refractivity misc Maximization misc Wavelengths |
| format_facet |
Aufsätze Gedruckte Aufsätze |
| format_main_str_mv |
Text Zeitschrift/Artikel |
| carriertype_str_mv |
nc |
| author2_variant |
b y by m e me n f a nf nfa |
| hierarchy_parent_title |
Optical and quantum electronics |
| hierarchy_parent_id |
129419540 |
| dewey-tens |
500 - Science 620 - Engineering |
| hierarchy_top_title |
Optical and quantum electronics |
| isfreeaccess_txt |
false |
| familylinks_str_mv |
(DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 |
| title |
Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
| ctrlnum |
(DE-627)OLC1996850040 (DE-599)GBVOLC1996850040 (PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590 (KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic |
| title_full |
Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
| author_sort |
Zaghloul, Seif eldin A |
| journal |
Optical and quantum electronics |
| journalStr |
Optical and quantum electronics |
| lang_code |
eng |
| isOA_bool |
false |
| dewey-hundreds |
500 - Science 600 - Technology |
| recordtype |
marc |
| publishDateSort |
2017 |
| contenttype_str_mv |
txt |
| container_start_page |
1 |
| author_browse |
Zaghloul, Seif eldin A |
| container_volume |
49 |
| class |
500 620 DE-600 33.38 bkl 33.18 bkl 33.23 bkl 53.54 bkl 52.88 bkl 33.72 bkl |
| format_se |
Aufsätze |
| author-letter |
Zaghloul, Seif eldin A |
| doi_str_mv |
10.1007/s11082-017-1180-7 |
| dewey-full |
500 620 |
| title_sort |
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 |
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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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 |
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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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 |
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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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. |
| collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 |
| container_issue |
11 |
| title_short |
Sensitivity maximization of leaky and weaky radiation micro/nano fiber sensors |
| url |
http://dx.doi.org/10.1007/s11082-017-1180-7 https://search.proquest.com/docview/1948153330 |
| remote_bool |
false |
| author2 |
Yousif, Bedir Elzalabani, Mahmoud Areed, Nehal Fayez |
| author2Str |
Yousif, Bedir Elzalabani, Mahmoud Areed, Nehal Fayez |
| ppnlink |
129419540 |
| mediatype_str_mv |
n |
| isOA_txt |
false |
| hochschulschrift_bool |
false |
| author2_role |
oth oth oth |
| doi_str |
10.1007/s11082-017-1180-7 |
| up_date |
2024-07-04T01:32:34.945Z |
| _version_ |
1803610231874256896 |
| fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a2200265 4500</leader><controlfield tag="001">OLC1996850040</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220219202958.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">171125s2017 xx ||||| 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="028" ind1="5" ind2="2"><subfield code="a">PQ20171228</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC1996850040</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVOLC1996850040</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(PRQ)p1311-5a92791e950429a213a24a888d5ca7a6165f0710136a7bb8e527ac9cb18545590</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(KEY)0014969120170000049001100001sensitivitymaximizationofleakyandweakyradiationmic</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">DE-600</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">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">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 (nf) for each environmental material (ne) with a specific wavelength (λmax) at which the highest sensitivity is achieved. Where the refractive indices nf and ne are wavelength dependent. For the leaky radiation microfiber sensor, the value of nf less than and getting close to the value of ne. 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 (Sθ) becomes very high with wavelength (λSθmax) at which nf ≈ ne. Such as, core (BK7 glass) and environmental (styrene) at λmax = 0.8 μm, the value of Sθ = 13759. In the weakly radiation, the value of nf greater than the value of ne. The sensitivity is evaluated by measurement the mode field radius (SW) or the fiber core power (SP). For core (BK7) and environmental (toluene) with core radius a = 1 μm, the sensitivity Sw = 2556 (μm/RIU) at λ = 1.75 μm and the sensitivity SP = 22.3 Pi (power unit/RIU) at λ = 1.05 μm (Pi is the fiber input power). The numerical evaluation of leaky radiation angle (θ) and sensitivity (Sθ) 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.</subfield></datafield><datafield tag="540" ind1=" " ind2=" "><subfield code="a">Nutzungsrecht: © Springer Science+Business Media, LLC, part of Springer Nature 2017</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Leaky radiation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Physics</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Computer Communication Networks</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Alcohols</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Electrical Engineering</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Petroleum productions</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Micro/nano fiber</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Optics, Lasers, Photonics, Optical Devices</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Weaky radiation</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Characterization and Evaluation of Materials</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Sensors</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Sensitivity analysis</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Toluene</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Refractivity</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Maximization</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Wavelengths</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Yousif, Bedir</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Elzalabani, Mahmoud</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Areed, Nehal Fayez</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Optical and quantum electronics</subfield><subfield code="d">Dordrecht : Kluwer, 1975</subfield><subfield code="g">49(2017), 11, Seite 1-21</subfield><subfield code="w">(DE-627)129419540</subfield><subfield code="w">(DE-600)189950-8</subfield><subfield code="w">(DE-576)014796139</subfield><subfield code="x">0306-8919</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:49</subfield><subfield code="g">year:2017</subfield><subfield code="g">number:11</subfield><subfield code="g">pages:1-21</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">http://dx.doi.org/10.1007/s11082-017-1180-7</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="856" ind1="4" ind2="2"><subfield code="u">https://search.proquest.com/docview/1948153330</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_150</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.38</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.18</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.23</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">53.54</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">52.88</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.72</subfield><subfield code="q">AVZ</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">49</subfield><subfield code="j">2017</subfield><subfield code="e">11</subfield><subfield code="h">1-21</subfield></datafield></record></collection>
|
| score |
7.4005175 |