Discriminating Bulk and Surface Refractive Index Changes With Fiber-Tip Leaky Mode Resonance
Optical surface wave excited by nanocoatings has enabled fiber-optic sensors with high sensitivity to the change in external environment generally characterized by bulk refractive index (RI). Nonetheless, this sensitive response inevitably suffers from the contamination of surface-localized binding...
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Veröffentlicht in: | Journal of lightwave technology 2023-07, Vol.41 (13), p.4341-4351 |
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creator | Li, Zhihong Yang, Xianxin Wang, Fei Zhu, Haiyong Jin, Xinxin Duan, Yanmin Chiavaioli, Francesco |
description | Optical surface wave excited by nanocoatings has enabled fiber-optic sensors with high sensitivity to the change in external environment generally characterized by bulk refractive index (RI). Nonetheless, this sensitive response inevitably suffers from the contamination of surface-localized binding events. Herein, we proposed and demonstrated a miniaturized fiber-tip leaky mode resonance ( {\rm {L^{e}MR}}) sensor capable of unambiguously discriminating bulk and surface RI changes from a theoretical perspective. The fiber-tip {\rm {L^{e}MR}} sensor consists of a multi-mode fiber tip coated with \mathrm{{TiO_{2}}} thin film on which a surface-localized binding layer thinner than 20 \, \rm nm was set equivalent to the change of surface RI. The operation principle was obtained, with the analyses revealing that several fiber-tip leaky modes can be excited with fiber core mode and flexibly tuned by simply altering the thickness of \mathrm{{TiO_{2}}} thin film, which hence generates non-polarized fiber-tip {\rm {L^{e}MRs}} identified by the signature of attenuation maxima in reflection spectrum of the fiber-tip probe. These fiber-tip {\rm {L^{e}MRs}} present a sensitive linear intensity response (and wavelength shift) to the change in bulk RI (and surface RI), which is considerably feasible for distinctly discriminating bulk and surface RI changes. The results highlight that both the highest bulk sensitivity up to 58.5 \, \mathrm{{dB/RIU}} in the RI range of 1.315 \sim 1.355 and the highest surface sensitivity up to 0.595 \, nm/nm, combined with the smallest cross interference between them, can be attained simultaneously with a single fiber-tip {\rm {L^{e}MR}} and without the need of ref |
doi_str_mv | 10.1109/JLT.2022.3187470 |
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fullrecord | <record><control><sourceid>proquest_RIE</sourceid><recordid>TN_cdi_ieee_primary_9811341</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><ieee_id>9811341</ieee_id><sourcerecordid>2839516066</sourcerecordid><originalsourceid>FETCH-LOGICAL-c291t-978296eb4442385d0d346e03f36a7af2d6586ebb2c0a53a7d198b8cb43e8e3293</originalsourceid><addsrcrecordid>eNo9kM9LwzAUx4MoOKd3wUvAc2d-tUmOOp1OKoJOvAghbV-3bJrOpBX339ux4ekd3vfzfbwPQueUjCgl-uoxn40YYWzEqZJCkgM0oGmqEsYoP0QDIjlPlGTiGJ3EuCSECqHkAH3culgG9-W8bZ2f45vuc4Wtr_BrF2pbAn6BOtiydT-Ap76CXzxeWD-HiN9du8ATV0BIZm6Nc7CrDX5qqi0SG299CafoqLafEc72c4jeJnez8UOSP99Px9d5UjJN20RLxXQGhRCCcZVWpOIiA8Jrnllpa1ZlqerXBSuJTbmVFdWqUGUhOCjgTPMhutz1rkPz3UFszbLpgu9PGqa4TmlGsqxPkV2qDE2MAWqz7h-3YWMoMVuHpndotg7N3mGPXOwQBwD_ca0o5YLyPxk4bAg</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2839516066</pqid></control><display><type>article</type><title>Discriminating Bulk and Surface Refractive Index Changes With Fiber-Tip Leaky Mode Resonance</title><source>IEEE Electronic Library (IEL)</source><creator>Li, Zhihong ; Yang, Xianxin ; Wang, Fei ; Zhu, Haiyong ; Jin, Xinxin ; Duan, Yanmin ; Chiavaioli, Francesco</creator><creatorcontrib>Li, Zhihong ; Yang, Xianxin ; Wang, Fei ; Zhu, Haiyong ; Jin, Xinxin ; Duan, Yanmin ; Chiavaioli, Francesco</creatorcontrib><description><![CDATA[Optical surface wave excited by nanocoatings has enabled fiber-optic sensors with high sensitivity to the change in external environment generally characterized by bulk refractive index (RI). Nonetheless, this sensitive response inevitably suffers from the contamination of surface-localized binding events. Herein, we proposed and demonstrated a miniaturized fiber-tip leaky mode resonance (<inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula>) sensor capable of unambiguously discriminating bulk and surface RI changes from a theoretical perspective. The fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula> sensor consists of a multi-mode fiber tip coated with <inline-formula><tex-math notation="LaTeX"> \mathrm{{TiO_{2}}}</tex-math></inline-formula> thin film on which a surface-localized binding layer thinner than <inline-formula><tex-math notation="LaTeX"> 20 \, \rm nm</tex-math></inline-formula> was set equivalent to the change of surface RI. The operation principle was obtained, with the analyses revealing that several fiber-tip leaky modes can be excited with fiber core mode and flexibly tuned by simply altering the thickness of <inline-formula><tex-math notation="LaTeX"> \mathrm{{TiO_{2}}}</tex-math></inline-formula> thin film, which hence generates non-polarized fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MRs}}</tex-math></inline-formula> identified by the signature of attenuation maxima in reflection spectrum of the fiber-tip probe. These fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MRs}}</tex-math></inline-formula> present a sensitive linear intensity response (and wavelength shift) to the change in bulk RI (and surface RI), which is considerably feasible for distinctly discriminating bulk and surface RI changes. The results highlight that both the highest bulk sensitivity up to <inline-formula><tex-math notation="LaTeX"> 58.5 \, \mathrm{{dB/RIU}}</tex-math></inline-formula> in the RI range of <inline-formula><tex-math notation="LaTeX"> 1.315 \sim 1.355</tex-math></inline-formula> and the highest surface sensitivity up to <inline-formula><tex-math notation="LaTeX"> 0.595 \, nm/nm</tex-math></inline-formula>, combined with the smallest cross interference between them, can be attained simultaneously with a single fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula> and without the need of reference channels, which could enable the development of ultra-compact lab-on-tip optrodes, a pathway of the lab-on-fiber roadmap.]]></description><identifier>ISSN: 0733-8724</identifier><identifier>EISSN: 1558-2213</identifier><identifier>DOI: 10.1109/JLT.2022.3187470</identifier><identifier>CODEN: JLTEDG</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Binding ; Biomedical optical imaging ; Bulk and surface refractive index ; Fiber optics ; lab-on-tip optrode ; leaky mode resonance ; Leaky modes ; Optical fiber sensors ; optical fiber tip ; Optical surface waves ; Refractivity ; Resonance ; Sensitivity ; Sensors ; Surface treatment ; Surface waves ; thin film ; Thin films</subject><ispartof>Journal of lightwave technology, 2023-07, Vol.41 (13), p.4341-4351</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2023</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c291t-978296eb4442385d0d346e03f36a7af2d6586ebb2c0a53a7d198b8cb43e8e3293</citedby><cites>FETCH-LOGICAL-c291t-978296eb4442385d0d346e03f36a7af2d6586ebb2c0a53a7d198b8cb43e8e3293</cites><orcidid>0000-0001-8606-3560 ; 0000-0002-3169-7395 ; 0000-0003-0655-0567 ; 0000-0002-7202-092X</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/9811341$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/9811341$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Li, Zhihong</creatorcontrib><creatorcontrib>Yang, Xianxin</creatorcontrib><creatorcontrib>Wang, Fei</creatorcontrib><creatorcontrib>Zhu, Haiyong</creatorcontrib><creatorcontrib>Jin, Xinxin</creatorcontrib><creatorcontrib>Duan, Yanmin</creatorcontrib><creatorcontrib>Chiavaioli, Francesco</creatorcontrib><title>Discriminating Bulk and Surface Refractive Index Changes With Fiber-Tip Leaky Mode Resonance</title><title>Journal of lightwave technology</title><addtitle>JLT</addtitle><description><![CDATA[Optical surface wave excited by nanocoatings has enabled fiber-optic sensors with high sensitivity to the change in external environment generally characterized by bulk refractive index (RI). Nonetheless, this sensitive response inevitably suffers from the contamination of surface-localized binding events. Herein, we proposed and demonstrated a miniaturized fiber-tip leaky mode resonance (<inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula>) sensor capable of unambiguously discriminating bulk and surface RI changes from a theoretical perspective. The fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula> sensor consists of a multi-mode fiber tip coated with <inline-formula><tex-math notation="LaTeX"> \mathrm{{TiO_{2}}}</tex-math></inline-formula> thin film on which a surface-localized binding layer thinner than <inline-formula><tex-math notation="LaTeX"> 20 \, \rm nm</tex-math></inline-formula> was set equivalent to the change of surface RI. The operation principle was obtained, with the analyses revealing that several fiber-tip leaky modes can be excited with fiber core mode and flexibly tuned by simply altering the thickness of <inline-formula><tex-math notation="LaTeX"> \mathrm{{TiO_{2}}}</tex-math></inline-formula> thin film, which hence generates non-polarized fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MRs}}</tex-math></inline-formula> identified by the signature of attenuation maxima in reflection spectrum of the fiber-tip probe. These fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MRs}}</tex-math></inline-formula> present a sensitive linear intensity response (and wavelength shift) to the change in bulk RI (and surface RI), which is considerably feasible for distinctly discriminating bulk and surface RI changes. The results highlight that both the highest bulk sensitivity up to <inline-formula><tex-math notation="LaTeX"> 58.5 \, \mathrm{{dB/RIU}}</tex-math></inline-formula> in the RI range of <inline-formula><tex-math notation="LaTeX"> 1.315 \sim 1.355</tex-math></inline-formula> and the highest surface sensitivity up to <inline-formula><tex-math notation="LaTeX"> 0.595 \, nm/nm</tex-math></inline-formula>, combined with the smallest cross interference between them, can be attained simultaneously with a single fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula> and without the need of reference channels, which could enable the development of ultra-compact lab-on-tip optrodes, a pathway of the lab-on-fiber roadmap.]]></description><subject>Binding</subject><subject>Biomedical optical imaging</subject><subject>Bulk and surface refractive index</subject><subject>Fiber optics</subject><subject>lab-on-tip optrode</subject><subject>leaky mode resonance</subject><subject>Leaky modes</subject><subject>Optical fiber sensors</subject><subject>optical fiber tip</subject><subject>Optical surface waves</subject><subject>Refractivity</subject><subject>Resonance</subject><subject>Sensitivity</subject><subject>Sensors</subject><subject>Surface treatment</subject><subject>Surface waves</subject><subject>thin film</subject><subject>Thin films</subject><issn>0733-8724</issn><issn>1558-2213</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNo9kM9LwzAUx4MoOKd3wUvAc2d-tUmOOp1OKoJOvAghbV-3bJrOpBX339ux4ekd3vfzfbwPQueUjCgl-uoxn40YYWzEqZJCkgM0oGmqEsYoP0QDIjlPlGTiGJ3EuCSECqHkAH3culgG9-W8bZ2f45vuc4Wtr_BrF2pbAn6BOtiydT-Ap76CXzxeWD-HiN9du8ATV0BIZm6Nc7CrDX5qqi0SG299CafoqLafEc72c4jeJnez8UOSP99Px9d5UjJN20RLxXQGhRCCcZVWpOIiA8Jrnllpa1ZlqerXBSuJTbmVFdWqUGUhOCjgTPMhutz1rkPz3UFszbLpgu9PGqa4TmlGsqxPkV2qDE2MAWqz7h-3YWMoMVuHpndotg7N3mGPXOwQBwD_ca0o5YLyPxk4bAg</recordid><startdate>20230701</startdate><enddate>20230701</enddate><creator>Li, Zhihong</creator><creator>Yang, Xianxin</creator><creator>Wang, Fei</creator><creator>Zhu, Haiyong</creator><creator>Jin, Xinxin</creator><creator>Duan, Yanmin</creator><creator>Chiavaioli, Francesco</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-8606-3560</orcidid><orcidid>https://orcid.org/0000-0002-3169-7395</orcidid><orcidid>https://orcid.org/0000-0003-0655-0567</orcidid><orcidid>https://orcid.org/0000-0002-7202-092X</orcidid></search><sort><creationdate>20230701</creationdate><title>Discriminating Bulk and Surface Refractive Index Changes With Fiber-Tip Leaky Mode Resonance</title><author>Li, Zhihong ; Yang, Xianxin ; Wang, Fei ; Zhu, Haiyong ; Jin, Xinxin ; Duan, Yanmin ; Chiavaioli, Francesco</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c291t-978296eb4442385d0d346e03f36a7af2d6586ebb2c0a53a7d198b8cb43e8e3293</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Binding</topic><topic>Biomedical optical imaging</topic><topic>Bulk and surface refractive index</topic><topic>Fiber optics</topic><topic>lab-on-tip optrode</topic><topic>leaky mode resonance</topic><topic>Leaky modes</topic><topic>Optical fiber sensors</topic><topic>optical fiber tip</topic><topic>Optical surface waves</topic><topic>Refractivity</topic><topic>Resonance</topic><topic>Sensitivity</topic><topic>Sensors</topic><topic>Surface treatment</topic><topic>Surface waves</topic><topic>thin film</topic><topic>Thin films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Li, Zhihong</creatorcontrib><creatorcontrib>Yang, Xianxin</creatorcontrib><creatorcontrib>Wang, Fei</creatorcontrib><creatorcontrib>Zhu, Haiyong</creatorcontrib><creatorcontrib>Jin, Xinxin</creatorcontrib><creatorcontrib>Duan, Yanmin</creatorcontrib><creatorcontrib>Chiavaioli, Francesco</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of lightwave technology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Li, Zhihong</au><au>Yang, Xianxin</au><au>Wang, Fei</au><au>Zhu, Haiyong</au><au>Jin, Xinxin</au><au>Duan, Yanmin</au><au>Chiavaioli, Francesco</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Discriminating Bulk and Surface Refractive Index Changes With Fiber-Tip Leaky Mode Resonance</atitle><jtitle>Journal of lightwave technology</jtitle><stitle>JLT</stitle><date>2023-07-01</date><risdate>2023</risdate><volume>41</volume><issue>13</issue><spage>4341</spage><epage>4351</epage><pages>4341-4351</pages><issn>0733-8724</issn><eissn>1558-2213</eissn><coden>JLTEDG</coden><abstract><![CDATA[Optical surface wave excited by nanocoatings has enabled fiber-optic sensors with high sensitivity to the change in external environment generally characterized by bulk refractive index (RI). Nonetheless, this sensitive response inevitably suffers from the contamination of surface-localized binding events. Herein, we proposed and demonstrated a miniaturized fiber-tip leaky mode resonance (<inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula>) sensor capable of unambiguously discriminating bulk and surface RI changes from a theoretical perspective. The fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula> sensor consists of a multi-mode fiber tip coated with <inline-formula><tex-math notation="LaTeX"> \mathrm{{TiO_{2}}}</tex-math></inline-formula> thin film on which a surface-localized binding layer thinner than <inline-formula><tex-math notation="LaTeX"> 20 \, \rm nm</tex-math></inline-formula> was set equivalent to the change of surface RI. The operation principle was obtained, with the analyses revealing that several fiber-tip leaky modes can be excited with fiber core mode and flexibly tuned by simply altering the thickness of <inline-formula><tex-math notation="LaTeX"> \mathrm{{TiO_{2}}}</tex-math></inline-formula> thin film, which hence generates non-polarized fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MRs}}</tex-math></inline-formula> identified by the signature of attenuation maxima in reflection spectrum of the fiber-tip probe. These fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MRs}}</tex-math></inline-formula> present a sensitive linear intensity response (and wavelength shift) to the change in bulk RI (and surface RI), which is considerably feasible for distinctly discriminating bulk and surface RI changes. The results highlight that both the highest bulk sensitivity up to <inline-formula><tex-math notation="LaTeX"> 58.5 \, \mathrm{{dB/RIU}}</tex-math></inline-formula> in the RI range of <inline-formula><tex-math notation="LaTeX"> 1.315 \sim 1.355</tex-math></inline-formula> and the highest surface sensitivity up to <inline-formula><tex-math notation="LaTeX"> 0.595 \, nm/nm</tex-math></inline-formula>, combined with the smallest cross interference between them, can be attained simultaneously with a single fiber-tip <inline-formula><tex-math notation="LaTeX"> {\rm {L^{e}MR}}</tex-math></inline-formula> and without the need of reference channels, which could enable the development of ultra-compact lab-on-tip optrodes, a pathway of the lab-on-fiber roadmap.]]></abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/JLT.2022.3187470</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0001-8606-3560</orcidid><orcidid>https://orcid.org/0000-0002-3169-7395</orcidid><orcidid>https://orcid.org/0000-0003-0655-0567</orcidid><orcidid>https://orcid.org/0000-0002-7202-092X</orcidid></addata></record> |
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subjects | Binding Biomedical optical imaging Bulk and surface refractive index Fiber optics lab-on-tip optrode leaky mode resonance Leaky modes Optical fiber sensors optical fiber tip Optical surface waves Refractivity Resonance Sensitivity Sensors Surface treatment Surface waves thin film Thin films |
title | Discriminating Bulk and Surface Refractive Index Changes With Fiber-Tip Leaky Mode Resonance |
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