Numerical analysis of plasmon polarition refractive index fiber sensors with hollow core and a long period grating
The main principle of this design is based on the efficient energy transfer between the waveguide mode (WM) and the co-directional SPP provided by a properly designed fiber long period grating (LPG). This LPG is imprinted into a waveguide fiber layer of a specially designed hollow core optical fiber...
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| Published in | Optics communications Vol. 284; no. 12; pp. 2835 - 2838 |
|---|---|
| Main Authors | , , , , |
| Format | Journal Article |
| Language | English |
| Published |
Elsevier B.V
01.06.2011
|
| Subjects | |
| Online Access | Get full text |
| ISSN | 0030-4018 1873-0310 |
| DOI | 10.1016/j.optcom.2011.02.034 |
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| Abstract | The main principle of this design is based on the efficient energy transfer between the waveguide mode (WM) and the co-directional SPP provided by a properly designed fiber long period grating (LPG). This LPG is imprinted into a waveguide fiber layer of a specially designed hollow core optical fiber. The simulations are based on the finite element method (FEM) algorithm in electromagnetics and coupled mode theory for gratings. Compared to the previous proposed structure using a fiber Bragg grating (FBG), this novel kind of sensor can greatly enhance the refractive index sensitivity, e.g., from 5.93
nm/RIU (with FBG) to 817
nm/RIU (with LPG) at the sensing refractive index of 1.40. The other advantage is that the working conditions can be performed for the well-developed telecom wavelength windows 1500–1600
nm.
► The efficient energy transfer between the waveguide mode (WM) and the co-directional SPP is investigated on a special hollow core optical fiber with a properly designed fiber long period grating (LPG). ► This novel kind of sensor can greatly enhance the refractive index sensitivity to 817 nm/RIU at the sensing refractive index of 1.40. ► The working conditions can be performed for the well-developed telecom wavelength windows 1500-1600 nm. |
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| AbstractList | The main principle of this design is based on the efficient energy transfer between the waveguide mode (WM) and the co-directional SPP provided by a properly designed fiber long period grating (LPG). This LPG is imprinted into a waveguide fiber layer of a specially designed hollow core optical fiber. The simulations are based on the finite element method (FEM) algorithm in electromagnetics and coupled mode theory for gratings. Compared to the previous proposed structure using a fiber Bragg grating (FBG), this novel kind of sensor can greatly enhance the refractive index sensitivity, e.g., from 5.93 nm/RIU (with FBG) to 817 nm/RIU (with LPG) at the sensing refractive index of 1.40. The other advantage is that the working conditions can be performed for the well-developed telecom wavelength windows 1500-1600 nm. The main principle of this design is based on the efficient energy transfer between the waveguide mode (WM) and the co-directional SPP provided by a properly designed fiber long period grating (LPG). This LPG is imprinted into a waveguide fiber layer of a specially designed hollow core optical fiber. The simulations are based on the finite element method (FEM) algorithm in electromagnetics and coupled mode theory for gratings. Compared to the previous proposed structure using a fiber Bragg grating (FBG), this novel kind of sensor can greatly enhance the refractive index sensitivity, e.g., from 5.93 nm/RIU (with FBG) to 817 nm/RIU (with LPG) at the sensing refractive index of 1.40. The other advantage is that the working conditions can be performed for the well-developed telecom wavelength windows 1500–1600 nm. ► The efficient energy transfer between the waveguide mode (WM) and the co-directional SPP is investigated on a special hollow core optical fiber with a properly designed fiber long period grating (LPG). ► This novel kind of sensor can greatly enhance the refractive index sensitivity to 817 nm/RIU at the sensing refractive index of 1.40. ► The working conditions can be performed for the well-developed telecom wavelength windows 1500-1600 nm. |
| Author | Liu, Deming Zhou, Chi Zhang, Yating Xia, Li Shuai, binbin |
| Author_xml | – sequence: 1 givenname: Li surname: Xia fullname: Xia, Li email: xiali@hust.edu.cn – sequence: 2 givenname: Yating surname: Zhang fullname: Zhang, Yating – sequence: 3 givenname: Chi surname: Zhou fullname: Zhou, Chi – sequence: 4 givenname: binbin surname: Shuai fullname: Shuai, binbin – sequence: 5 givenname: Deming surname: Liu fullname: Liu, Deming |
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| CitedBy_id | crossref_primary_10_1002_mop_27397 crossref_primary_10_1080_09500340_2015_1066455 crossref_primary_10_3390_s151127917 crossref_primary_10_1016_j_ijleo_2017_06_044 crossref_primary_10_1364_OE_24_010904 crossref_primary_10_1364_OE_26_000130 crossref_primary_10_1002_mop_28140 crossref_primary_10_1016_j_ijleo_2013_11_051 crossref_primary_10_1016_j_ijleo_2016_05_159 crossref_primary_10_1364_OE_21_032349 |
| Cites_doi | 10.1063/1.2360186 10.1016/j.optcom.2007.11.007 10.1117/1.2165171 10.1364/JOSAB.24.002696 10.1016/j.optcom.2005.04.066 10.1364/OE.14.011616 10.1109/JLT.2006.881464 10.1364/OE.14.010851 10.1364/JOSAB.24.001423 10.1007/s11468-008-9055-1 |
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| Keywords | Optical fiber sensors Fiber long period grating Surface plasmon polariton (SPP) Refractive index |
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| SubjectTerms | Computer simulation Diffraction gratings Fiber long period grating Fibers Finite element method Gratings (spectra) LPG Optical fiber sensors Refractive index Refractivity Surface plasmon polariton (SPP) |
| Title | Numerical analysis of plasmon polarition refractive index fiber sensors with hollow core and a long period grating |
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