Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance
Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is...
Ausführliche Beschreibung
Autor*in: |
Butt, Muhammad Ali [verfasserIn] |
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E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2022 |
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Anmerkung: |
© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 |
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Übergeordnetes Werk: |
Enthalten in: Plasmonics - New York, NY [u.a.] : Springer, 2006, 17(2022), 3 vom: 26. März, Seite 1305-1314 |
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Übergeordnetes Werk: |
volume:17 ; year:2022 ; number:3 ; day:26 ; month:03 ; pages:1305-1314 |
Links: |
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DOI / URN: |
10.1007/s11468-022-01633-8 |
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Katalog-ID: |
SPR047163070 |
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520 | |a Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. | ||
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650 | 4 | |a Refractive index sensor |7 (dpeaa)DE-He213 | |
650 | 4 | |a Temperature sensor |7 (dpeaa)DE-He213 | |
700 | 1 | |a Khonina, Svetlana Nikolaevna |4 aut | |
700 | 1 | |a Kazanskiy, Nikolay Lvovich |4 aut | |
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10.1007/s11468-022-01633-8 doi (DE-627)SPR047163070 (SPR)s11468-022-01633-8-e DE-627 ger DE-627 rakwb eng Butt, Muhammad Ali verfasserin (orcid)0000-0003-0829-4886 aut Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. Plasmonics (dpeaa)DE-He213 MIM waveguide (dpeaa)DE-He213 Refractive index sensor (dpeaa)DE-He213 Temperature sensor (dpeaa)DE-He213 Khonina, Svetlana Nikolaevna aut Kazanskiy, Nikolay Lvovich aut Enthalten in Plasmonics New York, NY [u.a.] : Springer, 2006 17(2022), 3 vom: 26. März, Seite 1305-1314 (DE-627)512879648 (DE-600)2237548-X 1557-1963 nnns volume:17 year:2022 number:3 day:26 month:03 pages:1305-1314 https://dx.doi.org/10.1007/s11468-022-01633-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 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_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 17 2022 3 26 03 1305-1314 |
spelling |
10.1007/s11468-022-01633-8 doi (DE-627)SPR047163070 (SPR)s11468-022-01633-8-e DE-627 ger DE-627 rakwb eng Butt, Muhammad Ali verfasserin (orcid)0000-0003-0829-4886 aut Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. Plasmonics (dpeaa)DE-He213 MIM waveguide (dpeaa)DE-He213 Refractive index sensor (dpeaa)DE-He213 Temperature sensor (dpeaa)DE-He213 Khonina, Svetlana Nikolaevna aut Kazanskiy, Nikolay Lvovich aut Enthalten in Plasmonics New York, NY [u.a.] : Springer, 2006 17(2022), 3 vom: 26. März, Seite 1305-1314 (DE-627)512879648 (DE-600)2237548-X 1557-1963 nnns volume:17 year:2022 number:3 day:26 month:03 pages:1305-1314 https://dx.doi.org/10.1007/s11468-022-01633-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 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_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 17 2022 3 26 03 1305-1314 |
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10.1007/s11468-022-01633-8 doi (DE-627)SPR047163070 (SPR)s11468-022-01633-8-e DE-627 ger DE-627 rakwb eng Butt, Muhammad Ali verfasserin (orcid)0000-0003-0829-4886 aut Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. Plasmonics (dpeaa)DE-He213 MIM waveguide (dpeaa)DE-He213 Refractive index sensor (dpeaa)DE-He213 Temperature sensor (dpeaa)DE-He213 Khonina, Svetlana Nikolaevna aut Kazanskiy, Nikolay Lvovich aut Enthalten in Plasmonics New York, NY [u.a.] : Springer, 2006 17(2022), 3 vom: 26. März, Seite 1305-1314 (DE-627)512879648 (DE-600)2237548-X 1557-1963 nnns volume:17 year:2022 number:3 day:26 month:03 pages:1305-1314 https://dx.doi.org/10.1007/s11468-022-01633-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 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_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 17 2022 3 26 03 1305-1314 |
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10.1007/s11468-022-01633-8 doi (DE-627)SPR047163070 (SPR)s11468-022-01633-8-e DE-627 ger DE-627 rakwb eng Butt, Muhammad Ali verfasserin (orcid)0000-0003-0829-4886 aut Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. Plasmonics (dpeaa)DE-He213 MIM waveguide (dpeaa)DE-He213 Refractive index sensor (dpeaa)DE-He213 Temperature sensor (dpeaa)DE-He213 Khonina, Svetlana Nikolaevna aut Kazanskiy, Nikolay Lvovich aut Enthalten in Plasmonics New York, NY [u.a.] : Springer, 2006 17(2022), 3 vom: 26. März, Seite 1305-1314 (DE-627)512879648 (DE-600)2237548-X 1557-1963 nnns volume:17 year:2022 number:3 day:26 month:03 pages:1305-1314 https://dx.doi.org/10.1007/s11468-022-01633-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 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_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 17 2022 3 26 03 1305-1314 |
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10.1007/s11468-022-01633-8 doi (DE-627)SPR047163070 (SPR)s11468-022-01633-8-e DE-627 ger DE-627 rakwb eng Butt, Muhammad Ali verfasserin (orcid)0000-0003-0829-4886 aut Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. Plasmonics (dpeaa)DE-He213 MIM waveguide (dpeaa)DE-He213 Refractive index sensor (dpeaa)DE-He213 Temperature sensor (dpeaa)DE-He213 Khonina, Svetlana Nikolaevna aut Kazanskiy, Nikolay Lvovich aut Enthalten in Plasmonics New York, NY [u.a.] : Springer, 2006 17(2022), 3 vom: 26. März, Seite 1305-1314 (DE-627)512879648 (DE-600)2237548-X 1557-1963 nnns volume:17 year:2022 number:3 day:26 month:03 pages:1305-1314 https://dx.doi.org/10.1007/s11468-022-01633-8 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 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_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 17 2022 3 26 03 1305-1314 |
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Butt, Muhammad Ali @@aut@@ Khonina, Svetlana Nikolaevna @@aut@@ Kazanskiy, Nikolay Lvovich @@aut@@ |
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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">SPR047163070</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230507194752.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">220602s2022 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11468-022-01633-8</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR047163070</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s11468-022-01633-8-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="100" ind1="1" ind2=" "><subfield code="a">Butt, Muhammad Ali</subfield><subfield code="e">verfasserin</subfield><subfield code="0">(orcid)0000-0003-0829-4886</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</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="500" ind1=" " ind2=" "><subfield code="a">© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. 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Butt, Muhammad Ali |
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simple and improved plasmonic sensor configuration established on mim waveguide for enhanced sensing performance |
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Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance |
abstract |
Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 |
abstractGer |
Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 |
abstract_unstemmed |
Abstract Herein, two simple configurations of Fano resonance-based plasmonic sensors are proposed for temperature and biosensing applications. The device optimization and sensing performance are numerically investigated via two-dimensional finite element method (2D-FEM). The former configuration is quite simple and based on the side-coupled circular cavity (SCCC), whereas in the latter, the circular cavity is encapsulated in the ring separated by a small gap and is known as ring encapsulated circular cavity (RECC). For temperature sensing applications, polydimethylsiloxane (PDMS) is utilized as a thermal sensing medium in the circular cavity. The numerical analysis has revealed that the temperature sensitivity (S) of SCCC and RECC configuration is ~ −0.58 nm/°C and −0.64 nm/°C, respectively. The figure of merit (FOM) is another important parameter to analyze the sensing performance which is around 8.6 and 1955.2 for SCCC and RECC configuration, respectively. The sensing capabilities of the biosensor designs are investigated by injecting dielectric materials of different refractive indices in the circular cavity ranges between 1.33 and 1.37. The S of the SCCC and RECC sensor configuration is around 1240 nm/RIU and 1350 nm/RIU, respectively, with a FOM of 18.74 $ RIU^{−1} $ and 691 $ RIU^{−1} $. The RECC sensor configuration is considered to be straightforward with fewer fabrication complications and offers high sensing performance. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022 |
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container_issue |
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title_short |
Simple and Improved Plasmonic Sensor Configuration Established on MIM Waveguide for Enhanced Sensing Performance |
url |
https://dx.doi.org/10.1007/s11468-022-01633-8 |
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Khonina, Svetlana Nikolaevna Kazanskiy, Nikolay Lvovich |
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Khonina, Svetlana Nikolaevna Kazanskiy, Nikolay Lvovich |
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10.1007/s11468-022-01633-8 |
up_date |
2024-07-04T02:07:54.932Z |
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score |
7.401531 |