Figure of merit enhancement of Ti3C2Tx-graphene based long-range surface plasmon sensor at telecommunication wavelength
In this work, the long-range surface plasmon resonance (LRSPR) sensor based on dielectric Ti 3 C 2 T x -graphene layers is demonstrated. Here, MXene (Ti 3 C 2 T x ) is used as a metal for strong surface plasmon’s generation at 1550 nm excitation wavelength. Graphene is used to attach the biomolecule...
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| Veröffentlicht in: | Optical and quantum electronics 2021-05, Vol.53 (5), Article 218 |
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| creator | Kumar, Rajeev Pal, Sarika Pal, Narendra Verma, Alka Saini, J. P. Prajapati, Yogendra Kumar |
| description | In this work, the long-range surface plasmon resonance (LRSPR) sensor based on dielectric Ti
3
C
2
T
x
-graphene layers is demonstrated. Here, MXene (Ti
3
C
2
T
x
) is used as a metal for strong surface plasmon’s generation at 1550 nm excitation wavelength. Graphene is used to attach the biomolecules having carbon–carbon structure with pi stacking interactions. The detection accuracy (DA) and figure of merit (FoM) for the proposed LRSPR sensor is theoretically investigated at telecommunication wavelength. The highest FoM of (559.64 RIU
−1
) is obtained at 3100 nm dielectric thickness and 14 nm Ti
3
C
2
T
x
thickness of the proposed sensor. The maximum improvement in FoM is 273% to the traditional LRSPR sensors. Propagation depths are also evaluated for Au-graphene and proposed LRSPR sensor at 14 and 27 nm thicknesses of Ti
3
C
2
T
x
We believe that the Ti
3
C
2
T
x
can be used in place of metals for strong plasmon generation in future sensor designs at telecommunication wavelengths. |
| doi_str_mv | 10.1007/s11082-021-02862-7 |
| format | Article |
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3
C
2
T
x
-graphene layers is demonstrated. Here, MXene (Ti
3
C
2
T
x
) is used as a metal for strong surface plasmon’s generation at 1550 nm excitation wavelength. Graphene is used to attach the biomolecules having carbon–carbon structure with pi stacking interactions. The detection accuracy (DA) and figure of merit (FoM) for the proposed LRSPR sensor is theoretically investigated at telecommunication wavelength. The highest FoM of (559.64 RIU
−1
) is obtained at 3100 nm dielectric thickness and 14 nm Ti
3
C
2
T
x
thickness of the proposed sensor. The maximum improvement in FoM is 273% to the traditional LRSPR sensors. Propagation depths are also evaluated for Au-graphene and proposed LRSPR sensor at 14 and 27 nm thicknesses of Ti
3
C
2
T
x
We believe that the Ti
3
C
2
T
x
can be used in place of metals for strong plasmon generation in future sensor designs at telecommunication wavelengths.</description><identifier>ISSN: 0306-8919</identifier><identifier>EISSN: 1572-817X</identifier><identifier>DOI: 10.1007/s11082-021-02862-7</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Biomolecules ; Carbon ; Characterization and Evaluation of Materials ; Computer Communication Networks ; Electrical Engineering ; Figure of merit ; Graphene ; Lasers ; Optical Devices ; Optics ; Photonics ; Physics ; Physics and Astronomy ; Sensors ; Thickness</subject><ispartof>Optical and quantum electronics, 2021-05, Vol.53 (5), Article 218</ispartof><rights>The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021</rights><rights>The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2021.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c319t-405a9bfc22cbdccda208c0e7b17a23f697baeaa90a7bc4ba2a2d126ea38037c73</citedby><cites>FETCH-LOGICAL-c319t-405a9bfc22cbdccda208c0e7b17a23f697baeaa90a7bc4ba2a2d126ea38037c73</cites><orcidid>0000-0002-6752-5667</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11082-021-02862-7$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11082-021-02862-7$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27901,27902,41464,42533,51294</link.rule.ids></links><search><creatorcontrib>Kumar, Rajeev</creatorcontrib><creatorcontrib>Pal, Sarika</creatorcontrib><creatorcontrib>Pal, Narendra</creatorcontrib><creatorcontrib>Verma, Alka</creatorcontrib><creatorcontrib>Saini, J. P.</creatorcontrib><creatorcontrib>Prajapati, Yogendra Kumar</creatorcontrib><title>Figure of merit enhancement of Ti3C2Tx-graphene based long-range surface plasmon sensor at telecommunication wavelength</title><title>Optical and quantum electronics</title><addtitle>Opt Quant Electron</addtitle><description>In this work, the long-range surface plasmon resonance (LRSPR) sensor based on dielectric Ti
3
C
2
T
x
-graphene layers is demonstrated. Here, MXene (Ti
3
C
2
T
x
) is used as a metal for strong surface plasmon’s generation at 1550 nm excitation wavelength. Graphene is used to attach the biomolecules having carbon–carbon structure with pi stacking interactions. The detection accuracy (DA) and figure of merit (FoM) for the proposed LRSPR sensor is theoretically investigated at telecommunication wavelength. The highest FoM of (559.64 RIU
−1
) is obtained at 3100 nm dielectric thickness and 14 nm Ti
3
C
2
T
x
thickness of the proposed sensor. The maximum improvement in FoM is 273% to the traditional LRSPR sensors. Propagation depths are also evaluated for Au-graphene and proposed LRSPR sensor at 14 and 27 nm thicknesses of Ti
3
C
2
T
x
We believe that the Ti
3
C
2
T
x
can be used in place of metals for strong plasmon generation in future sensor designs at telecommunication wavelengths.</description><subject>Biomolecules</subject><subject>Carbon</subject><subject>Characterization and Evaluation of Materials</subject><subject>Computer Communication Networks</subject><subject>Electrical Engineering</subject><subject>Figure of merit</subject><subject>Graphene</subject><subject>Lasers</subject><subject>Optical Devices</subject><subject>Optics</subject><subject>Photonics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Sensors</subject><subject>Thickness</subject><issn>0306-8919</issn><issn>1572-817X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNp9kEFLAzEQhYMoWKt_wFPAc3SStJvdoxSrQsFLBW9hNp3dbulma7Jr9d-bWsGbh2HgzXtv4GPsWsKtBDB3UUrIlQAl0-SZEuaEjeTUKJFL83bKRqAhE3khi3N2EeMGALLJFEZsP2_qIRDvKt5SaHpOfo3eUUu-P4jLRs_U8lPUAXdr8sRLjLTi287XIqCvicchVOiI77YY287zSD52gWPPe9qS69p28I3Dvkm3PX4kzdf9-pKdVbiNdPW7x-x1_rCcPYnFy-Pz7H4hnJZFLyYwxaKsnFKuXDm3QgW5AzKlNKh0lRWmREIsAE3pJiUqVCupMkKdgzbO6DG7OfbuQvc-UOztphuCTy-tmiZAWaYBkksdXS50MQaq7C40LYYvK8EeANsjYJsA2x_A9lCtj6GYzIlE-Kv-J_UNzDSA1w</recordid><startdate>20210501</startdate><enddate>20210501</enddate><creator>Kumar, Rajeev</creator><creator>Pal, Sarika</creator><creator>Pal, Narendra</creator><creator>Verma, Alka</creator><creator>Saini, J. P.</creator><creator>Prajapati, Yogendra Kumar</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-6752-5667</orcidid></search><sort><creationdate>20210501</creationdate><title>Figure of merit enhancement of Ti3C2Tx-graphene based long-range surface plasmon sensor at telecommunication wavelength</title><author>Kumar, Rajeev ; Pal, Sarika ; Pal, Narendra ; Verma, Alka ; Saini, J. P. ; Prajapati, Yogendra Kumar</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c319t-405a9bfc22cbdccda208c0e7b17a23f697baeaa90a7bc4ba2a2d126ea38037c73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Biomolecules</topic><topic>Carbon</topic><topic>Characterization and Evaluation of Materials</topic><topic>Computer Communication Networks</topic><topic>Electrical Engineering</topic><topic>Figure of merit</topic><topic>Graphene</topic><topic>Lasers</topic><topic>Optical Devices</topic><topic>Optics</topic><topic>Photonics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Sensors</topic><topic>Thickness</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kumar, Rajeev</creatorcontrib><creatorcontrib>Pal, Sarika</creatorcontrib><creatorcontrib>Pal, Narendra</creatorcontrib><creatorcontrib>Verma, Alka</creatorcontrib><creatorcontrib>Saini, J. P.</creatorcontrib><creatorcontrib>Prajapati, Yogendra Kumar</creatorcontrib><collection>CrossRef</collection><jtitle>Optical and quantum electronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kumar, Rajeev</au><au>Pal, Sarika</au><au>Pal, Narendra</au><au>Verma, Alka</au><au>Saini, J. P.</au><au>Prajapati, Yogendra Kumar</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Figure of merit enhancement of Ti3C2Tx-graphene based long-range surface plasmon sensor at telecommunication wavelength</atitle><jtitle>Optical and quantum electronics</jtitle><stitle>Opt Quant Electron</stitle><date>2021-05-01</date><risdate>2021</risdate><volume>53</volume><issue>5</issue><artnum>218</artnum><issn>0306-8919</issn><eissn>1572-817X</eissn><abstract>In this work, the long-range surface plasmon resonance (LRSPR) sensor based on dielectric Ti
3
C
2
T
x
-graphene layers is demonstrated. Here, MXene (Ti
3
C
2
T
x
) is used as a metal for strong surface plasmon’s generation at 1550 nm excitation wavelength. Graphene is used to attach the biomolecules having carbon–carbon structure with pi stacking interactions. The detection accuracy (DA) and figure of merit (FoM) for the proposed LRSPR sensor is theoretically investigated at telecommunication wavelength. The highest FoM of (559.64 RIU
−1
) is obtained at 3100 nm dielectric thickness and 14 nm Ti
3
C
2
T
x
thickness of the proposed sensor. The maximum improvement in FoM is 273% to the traditional LRSPR sensors. Propagation depths are also evaluated for Au-graphene and proposed LRSPR sensor at 14 and 27 nm thicknesses of Ti
3
C
2
T
x
We believe that the Ti
3
C
2
T
x
can be used in place of metals for strong plasmon generation in future sensor designs at telecommunication wavelengths.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s11082-021-02862-7</doi><orcidid>https://orcid.org/0000-0002-6752-5667</orcidid></addata></record> |
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| issn | 0306-8919 1572-817X |
| language | eng |
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| source | Springer Nature - Complete Springer Journals |
| subjects | Biomolecules Carbon Characterization and Evaluation of Materials Computer Communication Networks Electrical Engineering Figure of merit Graphene Lasers Optical Devices Optics Photonics Physics Physics and Astronomy Sensors Thickness |
| title | Figure of merit enhancement of Ti3C2Tx-graphene based long-range surface plasmon sensor at telecommunication wavelength |
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