Localized Refractive index sensing by integrated photonic crystal waveguide with edge-cavity
We have theoretically proposed a highly compact refractive-index sensor consisted of edge-cavity and line-defect waveguide in two-dimensional photonic crystal. The sensing object is completely outside of the single enclosed surface of the sensor. The edge-cavity is designed by engineering the spatia...
Gespeichert in:
Veröffentlicht in: | arXiv.org 2023-09 |
---|---|
Hauptverfasser: | , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | |
---|---|
container_issue | |
container_start_page | |
container_title | arXiv.org |
container_volume | |
creator | Luo, Ma Zhong, Kaichan Luo, Jieli |
description | We have theoretically proposed a highly compact refractive-index sensor consisted of edge-cavity and line-defect waveguide in two-dimensional photonic crystal. The sensing object is completely outside of the single enclosed surface of the sensor. The edge-cavity is designed by engineering the spatial distribution of the cutoff frequency of edge modes. The coupling between the edge-cavity and the waveguide is maximized by optimizing the radius of the rods between them, so that the transmittance spectrum through the waveguide has a sharp anti-peak. As the refractive index of the sensing object changes, the resonant wavelength of the edge-cavity is changed, which in turn changes the wavelength of the anti-peak. The sensitivity of the sensor is up to 40 nm/RIU, and the footprint of the sensor is only 40 \(\mu m^{2}\). Because the transmittance spectrum is determined by the overlap between the sensing object and the highly localized resonant mode, the sensor can also perceive spatial distribution of refractive index in the sensing object. |
format | Article |
fullrecord | <record><control><sourceid>proquest</sourceid><recordid>TN_cdi_proquest_journals_2828087945</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2828087945</sourcerecordid><originalsourceid>FETCH-proquest_journals_28280879453</originalsourceid><addsrcrecordid>eNqNikELgjAYQEcQJOV_GHQW1tRc5yg6dIqOgaztc05ks21q9uvz0A_o9OC9t0ARTdNdwjJKVyj2viGE0H1B8zyN0ONqBW_1ByS-QeW4CHoArI2EN_ZgvDYKP6dZBFCOh3nrahus0QILN_nAWzzyAVSvJeBRhxqDVJAIPugwbdCy4q2H-Mc12p5P9-Ml6Zx99eBD2djemTmVlFFGWHHI8vS_6wtEgERz</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2828087945</pqid></control><display><type>article</type><title>Localized Refractive index sensing by integrated photonic crystal waveguide with edge-cavity</title><source>Free E- Journals</source><creator>Luo, Ma ; Zhong, Kaichan ; Luo, Jieli</creator><creatorcontrib>Luo, Ma ; Zhong, Kaichan ; Luo, Jieli</creatorcontrib><description>We have theoretically proposed a highly compact refractive-index sensor consisted of edge-cavity and line-defect waveguide in two-dimensional photonic crystal. The sensing object is completely outside of the single enclosed surface of the sensor. The edge-cavity is designed by engineering the spatial distribution of the cutoff frequency of edge modes. The coupling between the edge-cavity and the waveguide is maximized by optimizing the radius of the rods between them, so that the transmittance spectrum through the waveguide has a sharp anti-peak. As the refractive index of the sensing object changes, the resonant wavelength of the edge-cavity is changed, which in turn changes the wavelength of the anti-peak. The sensitivity of the sensor is up to 40 nm/RIU, and the footprint of the sensor is only 40 \(\mu m^{2}\). Because the transmittance spectrum is determined by the overlap between the sensing object and the highly localized resonant mode, the sensor can also perceive spatial distribution of refractive index in the sensing object.</description><identifier>EISSN: 2331-8422</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Circuits ; Coupled modes ; Coupling ; Crystal defects ; Optical communication ; Photonic crystals ; Point defects ; Refractivity ; Spatial distribution ; Transmittance ; Waveguides</subject><ispartof>arXiv.org, 2023-09</ispartof><rights>2023. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>780,784</link.rule.ids></links><search><creatorcontrib>Luo, Ma</creatorcontrib><creatorcontrib>Zhong, Kaichan</creatorcontrib><creatorcontrib>Luo, Jieli</creatorcontrib><title>Localized Refractive index sensing by integrated photonic crystal waveguide with edge-cavity</title><title>arXiv.org</title><description>We have theoretically proposed a highly compact refractive-index sensor consisted of edge-cavity and line-defect waveguide in two-dimensional photonic crystal. The sensing object is completely outside of the single enclosed surface of the sensor. The edge-cavity is designed by engineering the spatial distribution of the cutoff frequency of edge modes. The coupling between the edge-cavity and the waveguide is maximized by optimizing the radius of the rods between them, so that the transmittance spectrum through the waveguide has a sharp anti-peak. As the refractive index of the sensing object changes, the resonant wavelength of the edge-cavity is changed, which in turn changes the wavelength of the anti-peak. The sensitivity of the sensor is up to 40 nm/RIU, and the footprint of the sensor is only 40 \(\mu m^{2}\). Because the transmittance spectrum is determined by the overlap between the sensing object and the highly localized resonant mode, the sensor can also perceive spatial distribution of refractive index in the sensing object.</description><subject>Circuits</subject><subject>Coupled modes</subject><subject>Coupling</subject><subject>Crystal defects</subject><subject>Optical communication</subject><subject>Photonic crystals</subject><subject>Point defects</subject><subject>Refractivity</subject><subject>Spatial distribution</subject><subject>Transmittance</subject><subject>Waveguides</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNqNikELgjAYQEcQJOV_GHQW1tRc5yg6dIqOgaztc05ks21q9uvz0A_o9OC9t0ARTdNdwjJKVyj2viGE0H1B8zyN0ONqBW_1ByS-QeW4CHoArI2EN_ZgvDYKP6dZBFCOh3nrahus0QILN_nAWzzyAVSvJeBRhxqDVJAIPugwbdCy4q2H-Mc12p5P9-Ml6Zx99eBD2djemTmVlFFGWHHI8vS_6wtEgERz</recordid><startdate>20230921</startdate><enddate>20230921</enddate><creator>Luo, Ma</creator><creator>Zhong, Kaichan</creator><creator>Luo, Jieli</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PTHSS</scope></search><sort><creationdate>20230921</creationdate><title>Localized Refractive index sensing by integrated photonic crystal waveguide with edge-cavity</title><author>Luo, Ma ; Zhong, Kaichan ; Luo, Jieli</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_28280879453</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Circuits</topic><topic>Coupled modes</topic><topic>Coupling</topic><topic>Crystal defects</topic><topic>Optical communication</topic><topic>Photonic crystals</topic><topic>Point defects</topic><topic>Refractivity</topic><topic>Spatial distribution</topic><topic>Transmittance</topic><topic>Waveguides</topic><toplevel>online_resources</toplevel><creatorcontrib>Luo, Ma</creatorcontrib><creatorcontrib>Zhong, Kaichan</creatorcontrib><creatorcontrib>Luo, Jieli</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>Engineering Collection</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Luo, Ma</au><au>Zhong, Kaichan</au><au>Luo, Jieli</au><format>book</format><genre>document</genre><ristype>GEN</ristype><atitle>Localized Refractive index sensing by integrated photonic crystal waveguide with edge-cavity</atitle><jtitle>arXiv.org</jtitle><date>2023-09-21</date><risdate>2023</risdate><eissn>2331-8422</eissn><abstract>We have theoretically proposed a highly compact refractive-index sensor consisted of edge-cavity and line-defect waveguide in two-dimensional photonic crystal. The sensing object is completely outside of the single enclosed surface of the sensor. The edge-cavity is designed by engineering the spatial distribution of the cutoff frequency of edge modes. The coupling between the edge-cavity and the waveguide is maximized by optimizing the radius of the rods between them, so that the transmittance spectrum through the waveguide has a sharp anti-peak. As the refractive index of the sensing object changes, the resonant wavelength of the edge-cavity is changed, which in turn changes the wavelength of the anti-peak. The sensitivity of the sensor is up to 40 nm/RIU, and the footprint of the sensor is only 40 \(\mu m^{2}\). Because the transmittance spectrum is determined by the overlap between the sensing object and the highly localized resonant mode, the sensor can also perceive spatial distribution of refractive index in the sensing object.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | EISSN: 2331-8422 |
ispartof | arXiv.org, 2023-09 |
issn | 2331-8422 |
language | eng |
recordid | cdi_proquest_journals_2828087945 |
source | Free E- Journals |
subjects | Circuits Coupled modes Coupling Crystal defects Optical communication Photonic crystals Point defects Refractivity Spatial distribution Transmittance Waveguides |
title | Localized Refractive index sensing by integrated photonic crystal waveguide with edge-cavity |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-05T14%3A34%3A09IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest&rft_val_fmt=info:ofi/fmt:kev:mtx:book&rft.genre=document&rft.atitle=Localized%20Refractive%20index%20sensing%20by%20integrated%20photonic%20crystal%20waveguide%20with%20edge-cavity&rft.jtitle=arXiv.org&rft.au=Luo,%20Ma&rft.date=2023-09-21&rft.eissn=2331-8422&rft_id=info:doi/&rft_dat=%3Cproquest%3E2828087945%3C/proquest%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2828087945&rft_id=info:pmid/&rfr_iscdi=true |