Higher Q factor and higher extinction ratio with lower detection limit photonic crystal-parallel-integrated sensor array for on-chip optical multiplexing sensing
We introduce an alternative method to establish a nanoscale sensor array based on a photonic crystal (PhC) slab, which is referred to as a 1×4 monolithic PhC parallel-integrated sensor array (PhC-PISA). To realize this function, four lattice-shifted resonant cavities are butt-coupled to four output...
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Veröffentlicht in: | Applied Optics 2016-12, Vol.55 (35), p.10078-10083 |
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creator | Zhou, Jian Huang, Lijun Fu, Zhongyuan Sun, Fujun Tian, Huiping |
description | We introduce an alternative method to establish a nanoscale sensor array based on a photonic crystal (PhC) slab, which is referred to as a 1×4 monolithic PhC parallel-integrated sensor array (PhC-PISA). To realize this function, four lattice-shifted resonant cavities are butt-coupled to four output waveguide branches, respectively. By shifting the first to the two closest neighboring holes around the defect, a high Q factor over 1.5×10
has been obtained. Owing to the slightly different cavity spacing, each PhC resonator shows an independent resonant peak shift as the refractive index changes surrounding the resonant cavity. The specific single peak with a well-defined extinction ratio exceeds 25 dB. By applying the finite-difference time-domain (FDTD) method, we demonstrate that the sensitivities of each sensor in PhC-PISA S
=60.500 nm/RIU, S
=59.623 nm/RIU, S
=62.500 nm/RIU, and S
=51.142 nm/RIU (refractive index unit) are achieved, respectively. In addition, the negligible crosstalk and detection limit as small as 1×10
have been observed. The proposed sensor array as a desirable platform has great potential to realize optical multiplexing sensing and high-density monolithic integration. |
doi_str_mv | 10.1364/AO.55.010078 |
format | Article |
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has been obtained. Owing to the slightly different cavity spacing, each PhC resonator shows an independent resonant peak shift as the refractive index changes surrounding the resonant cavity. The specific single peak with a well-defined extinction ratio exceeds 25 dB. By applying the finite-difference time-domain (FDTD) method, we demonstrate that the sensitivities of each sensor in PhC-PISA S
=60.500 nm/RIU, S
=59.623 nm/RIU, S
=62.500 nm/RIU, and S
=51.142 nm/RIU (refractive index unit) are achieved, respectively. In addition, the negligible crosstalk and detection limit as small as 1×10
have been observed. The proposed sensor array as a desirable platform has great potential to realize optical multiplexing sensing and high-density monolithic integration.</description><identifier>ISSN: 0003-6935</identifier><identifier>ISSN: 1559-128X</identifier><identifier>EISSN: 2155-3165</identifier><identifier>EISSN: 1539-4522</identifier><identifier>DOI: 10.1364/AO.55.010078</identifier><identifier>PMID: 27958421</identifier><language>eng</language><publisher>United States</publisher><subject>Detection ; Extinction ; Holes ; Multiplexing ; Q factors ; Refractive index ; Refractivity ; Sensor arrays</subject><ispartof>Applied Optics, 2016-12, Vol.55 (35), p.10078-10083</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c254t-60bd82c1b235c2e4601ad3885f656a092c11ff3531a09392c54896f3609127793</citedby><cites>FETCH-LOGICAL-c254t-60bd82c1b235c2e4601ad3885f656a092c11ff3531a09392c54896f3609127793</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/27958421$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Zhou, Jian</creatorcontrib><creatorcontrib>Huang, Lijun</creatorcontrib><creatorcontrib>Fu, Zhongyuan</creatorcontrib><creatorcontrib>Sun, Fujun</creatorcontrib><creatorcontrib>Tian, Huiping</creatorcontrib><title>Higher Q factor and higher extinction ratio with lower detection limit photonic crystal-parallel-integrated sensor array for on-chip optical multiplexing sensing</title><title>Applied Optics</title><addtitle>Appl Opt</addtitle><description>We introduce an alternative method to establish a nanoscale sensor array based on a photonic crystal (PhC) slab, which is referred to as a 1×4 monolithic PhC parallel-integrated sensor array (PhC-PISA). To realize this function, four lattice-shifted resonant cavities are butt-coupled to four output waveguide branches, respectively. By shifting the first to the two closest neighboring holes around the defect, a high Q factor over 1.5×10
has been obtained. Owing to the slightly different cavity spacing, each PhC resonator shows an independent resonant peak shift as the refractive index changes surrounding the resonant cavity. The specific single peak with a well-defined extinction ratio exceeds 25 dB. By applying the finite-difference time-domain (FDTD) method, we demonstrate that the sensitivities of each sensor in PhC-PISA S
=60.500 nm/RIU, S
=59.623 nm/RIU, S
=62.500 nm/RIU, and S
=51.142 nm/RIU (refractive index unit) are achieved, respectively. In addition, the negligible crosstalk and detection limit as small as 1×10
have been observed. The proposed sensor array as a desirable platform has great potential to realize optical multiplexing sensing and high-density monolithic integration.</description><subject>Detection</subject><subject>Extinction</subject><subject>Holes</subject><subject>Multiplexing</subject><subject>Q factors</subject><subject>Refractive index</subject><subject>Refractivity</subject><subject>Sensor arrays</subject><issn>0003-6935</issn><issn>1559-128X</issn><issn>2155-3165</issn><issn>1539-4522</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqNkc1O3DAUha2qVRlod10jL7topv7JdeLlCNGChDSq1K4jj-NMjBw72B7BPA5vimmANatzj893rxcHoW-UrCkX9c_Ndg2wJpSQpv2AVowCVJwK-IhWhBBeCcnhBJ2mdFsc1LL5jE5YI6GtGV2hxyu7H03Ef_CgdA4RK9_jcXkzD9l6nW3wOKoi-N7mEbtwX7LeZLNEzk4243kMOXirsY7HlJWrZhWVc8ZV1mezL_umx8n49PxFjOqIhzIFX-nRzjjM2Wrl8HRw2c7OPFi__08X_YI-Dcol8_VFz9C_X5d_L66qm-3v64vNTaUZ1LkSZNe3TNMd46CZqQWhqudtC4MAoYgsER0GDpwWw4uFupVi4IJIyppG8jP0fbk7x3B3MCl3k03aOKe8CYfU0baRUjZSkHegwIRoaQMF_bGgOoaUohm6OdpJxWNHSffcX7fZdgDd0l_Bz18uH3aT6d_g18L4EwUzl9c</recordid><startdate>20161210</startdate><enddate>20161210</enddate><creator>Zhou, Jian</creator><creator>Huang, Lijun</creator><creator>Fu, Zhongyuan</creator><creator>Sun, Fujun</creator><creator>Tian, Huiping</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20161210</creationdate><title>Higher Q factor and higher extinction ratio with lower detection limit photonic crystal-parallel-integrated sensor array for on-chip optical multiplexing sensing</title><author>Zhou, Jian ; Huang, Lijun ; Fu, Zhongyuan ; Sun, Fujun ; Tian, Huiping</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c254t-60bd82c1b235c2e4601ad3885f656a092c11ff3531a09392c54896f3609127793</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Detection</topic><topic>Extinction</topic><topic>Holes</topic><topic>Multiplexing</topic><topic>Q factors</topic><topic>Refractive index</topic><topic>Refractivity</topic><topic>Sensor arrays</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zhou, Jian</creatorcontrib><creatorcontrib>Huang, Lijun</creatorcontrib><creatorcontrib>Fu, Zhongyuan</creatorcontrib><creatorcontrib>Sun, Fujun</creatorcontrib><creatorcontrib>Tian, Huiping</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</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>Applied Optics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhou, Jian</au><au>Huang, Lijun</au><au>Fu, Zhongyuan</au><au>Sun, Fujun</au><au>Tian, Huiping</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Higher Q factor and higher extinction ratio with lower detection limit photonic crystal-parallel-integrated sensor array for on-chip optical multiplexing sensing</atitle><jtitle>Applied Optics</jtitle><addtitle>Appl Opt</addtitle><date>2016-12-10</date><risdate>2016</risdate><volume>55</volume><issue>35</issue><spage>10078</spage><epage>10083</epage><pages>10078-10083</pages><issn>0003-6935</issn><issn>1559-128X</issn><eissn>2155-3165</eissn><eissn>1539-4522</eissn><abstract>We introduce an alternative method to establish a nanoscale sensor array based on a photonic crystal (PhC) slab, which is referred to as a 1×4 monolithic PhC parallel-integrated sensor array (PhC-PISA). To realize this function, four lattice-shifted resonant cavities are butt-coupled to four output waveguide branches, respectively. By shifting the first to the two closest neighboring holes around the defect, a high Q factor over 1.5×10
has been obtained. Owing to the slightly different cavity spacing, each PhC resonator shows an independent resonant peak shift as the refractive index changes surrounding the resonant cavity. The specific single peak with a well-defined extinction ratio exceeds 25 dB. By applying the finite-difference time-domain (FDTD) method, we demonstrate that the sensitivities of each sensor in PhC-PISA S
=60.500 nm/RIU, S
=59.623 nm/RIU, S
=62.500 nm/RIU, and S
=51.142 nm/RIU (refractive index unit) are achieved, respectively. In addition, the negligible crosstalk and detection limit as small as 1×10
have been observed. The proposed sensor array as a desirable platform has great potential to realize optical multiplexing sensing and high-density monolithic integration.</abstract><cop>United States</cop><pmid>27958421</pmid><doi>10.1364/AO.55.010078</doi><tpages>6</tpages></addata></record> |
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source | Alma/SFX Local Collection; Optica Publishing Group Journals |
subjects | Detection Extinction Holes Multiplexing Q factors Refractive index Refractivity Sensor arrays |
title | Higher Q factor and higher extinction ratio with lower detection limit photonic crystal-parallel-integrated sensor array for on-chip optical multiplexing sensing |
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