Characterization of Porous Silicon Fabry-Pérot Optical Sensors for Reflectivity and Transmittivity Measurements
We investigate the effect of fabrication parameters (nonequal surface current densities, impurities inside the structure, etc.) and loss factor on reflectivity and transmittivity measurements from porous silicon Fabry-Pérot cavities with finite-size substrate thicknesses. We apply the formalism bas...
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Veröffentlicht in: | IEEE journal of selected topics in quantum electronics 2015-07, Vol.21 (4), p.174-183 |
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creator | Hasar, Ugur C. Ozbek, Ibrahim Y. Cavusoglu, Bulent Karacali, Tevhit Efeoglu, Hasan Ertugrul, Mehmet Barroso, Joaquim Jose |
description | We investigate the effect of fabrication parameters (nonequal surface current densities, impurities inside the structure, etc.) and loss factor on reflectivity and transmittivity measurements from porous silicon Fabry-Pérot cavities with finite-size substrate thicknesses. We apply the formalism based on wave cascade matrix method for obtaining dependencies of reflectivity and transmittivity. From our analysis, we note the following results. First, resonance behavior of reflectivity and transmittivity changes only when optical/physical properties of middle layers of the cavity alter. Second, for lossless cavities, while reflectivity and transmittivity considerably change with surface characteristics (optical/physical properties of first layers), transmittivity is significantly modified by a change of optical/physical properties of middle layers (microcavity region). Third, loss inside a FP cavity makes the transmittivity more immune to variations in optical/physical properties of middle layers. Finally and most importantly, transmittivity values at resonance wavelength as well as the resonance wavelength shift can be utilized for the identification of unknown chemical/biological molecules by lossless FP cavities. For validation of these results, we carried out reflectivity and transmittivity measurements from some arbitrarily chosen positions but around the center of two fabricated FP cavities resonating at 1456 nm and at 542 nm. |
doi_str_mv | 10.1109/JSTQE.2014.2365583 |
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We apply the formalism based on wave cascade matrix method for obtaining dependencies of reflectivity and transmittivity. From our analysis, we note the following results. First, resonance behavior of reflectivity and transmittivity changes only when optical/physical properties of middle layers of the cavity alter. Second, for lossless cavities, while reflectivity and transmittivity considerably change with surface characteristics (optical/physical properties of first layers), transmittivity is significantly modified by a change of optical/physical properties of middle layers (microcavity region). Third, loss inside a FP cavity makes the transmittivity more immune to variations in optical/physical properties of middle layers. Finally and most importantly, transmittivity values at resonance wavelength as well as the resonance wavelength shift can be utilized for the identification of unknown chemical/biological molecules by lossless FP cavities. For validation of these results, we carried out reflectivity and transmittivity measurements from some arbitrarily chosen positions but around the center of two fabricated FP cavities resonating at 1456 nm and at 542 nm.</description><identifier>ISSN: 1077-260X</identifier><identifier>EISSN: 1558-4542</identifier><identifier>DOI: 10.1109/JSTQE.2014.2365583</identifier><identifier>CODEN: IJSQEN</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Cavity resonators ; characterization ; Fabry-Perot cavity ; Filled plastics ; Holes ; Lossless ; Optical losses ; Optical properties ; Optical sensors ; Physical properties ; Porous silicon ; Propagation losses ; Reflectivity ; Refractive index ; Silicon ; Substrates ; transmittivity ; Wavelengths</subject><ispartof>IEEE journal of selected topics in quantum electronics, 2015-07, Vol.21 (4), p.174-183</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) Jul 2015</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c328t-661f948f68b2fd3f72f1f97e0eccbd0e8a75f6f1abaad05d4f0dc9ce035626873</citedby><cites>FETCH-LOGICAL-c328t-661f948f68b2fd3f72f1f97e0eccbd0e8a75f6f1abaad05d4f0dc9ce035626873</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/6940221$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/6940221$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Hasar, Ugur C.</creatorcontrib><creatorcontrib>Ozbek, Ibrahim Y.</creatorcontrib><creatorcontrib>Cavusoglu, Bulent</creatorcontrib><creatorcontrib>Karacali, Tevhit</creatorcontrib><creatorcontrib>Efeoglu, Hasan</creatorcontrib><creatorcontrib>Ertugrul, Mehmet</creatorcontrib><creatorcontrib>Barroso, Joaquim Jose</creatorcontrib><title>Characterization of Porous Silicon Fabry-Pérot Optical Sensors for Reflectivity and Transmittivity Measurements</title><title>IEEE journal of selected topics in quantum electronics</title><addtitle>JSTQE</addtitle><description>We investigate the effect of fabrication parameters (nonequal surface current densities, impurities inside the structure, etc.) and loss factor on reflectivity and transmittivity measurements from porous silicon Fabry-Pérot cavities with finite-size substrate thicknesses. We apply the formalism based on wave cascade matrix method for obtaining dependencies of reflectivity and transmittivity. From our analysis, we note the following results. First, resonance behavior of reflectivity and transmittivity changes only when optical/physical properties of middle layers of the cavity alter. Second, for lossless cavities, while reflectivity and transmittivity considerably change with surface characteristics (optical/physical properties of first layers), transmittivity is significantly modified by a change of optical/physical properties of middle layers (microcavity region). Third, loss inside a FP cavity makes the transmittivity more immune to variations in optical/physical properties of middle layers. Finally and most importantly, transmittivity values at resonance wavelength as well as the resonance wavelength shift can be utilized for the identification of unknown chemical/biological molecules by lossless FP cavities. For validation of these results, we carried out reflectivity and transmittivity measurements from some arbitrarily chosen positions but around the center of two fabricated FP cavities resonating at 1456 nm and at 542 nm.</description><subject>Cavity resonators</subject><subject>characterization</subject><subject>Fabry-Perot cavity</subject><subject>Filled plastics</subject><subject>Holes</subject><subject>Lossless</subject><subject>Optical losses</subject><subject>Optical properties</subject><subject>Optical sensors</subject><subject>Physical properties</subject><subject>Porous silicon</subject><subject>Propagation losses</subject><subject>Reflectivity</subject><subject>Refractive index</subject><subject>Silicon</subject><subject>Substrates</subject><subject>transmittivity</subject><subject>Wavelengths</subject><issn>1077-260X</issn><issn>1558-4542</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNpdUctOwzAQjBBIQOEH4GKJC5eUtZ04yRFVLQ-BCrRI3CLXWQujNC62i1T-iO_gx3BpxYHTrEYzo92dJDmh0KcUqovbyfRx2GdAsz7jIs9LvpMc0IhplmdsN85QFCkT8LKfHHr_BgBlVsJBshi8SidVQGc-ZTC2I1aTB-vs0pOJaY2KzEjO3Cp9-P5yNpDxIhglWzLBzlvnibaOPKFuUQXzYcKKyK4hUyc7PzdhS92j9EuHc-yCP0r2tGw9Hm-xlzyPhtPBdXo3vroZXN6lirMypEJQXWWlFuWM6YbrgulIFAio1KwBLGWRa6GpnEnZQN5kGhpVKQSeCybKgveS803uwtn3JfpQz41X2Layw3hcTUVOeVUITqP07J_0zS5dF7eLKhHfxCpYB7KNSjnrvUNdL5yZS7eqKdTrEurfEup1CfW2hGg63ZgMIv4ZRJUBY5T_AD7ahqM</recordid><startdate>201507</startdate><enddate>201507</enddate><creator>Hasar, Ugur C.</creator><creator>Ozbek, Ibrahim Y.</creator><creator>Cavusoglu, Bulent</creator><creator>Karacali, Tevhit</creator><creator>Efeoglu, Hasan</creator><creator>Ertugrul, Mehmet</creator><creator>Barroso, Joaquim Jose</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>L7M</scope><scope>F28</scope><scope>FR3</scope></search><sort><creationdate>201507</creationdate><title>Characterization of Porous Silicon Fabry-Pérot Optical Sensors for Reflectivity and Transmittivity Measurements</title><author>Hasar, Ugur C. ; Ozbek, Ibrahim Y. ; Cavusoglu, Bulent ; Karacali, Tevhit ; Efeoglu, Hasan ; Ertugrul, Mehmet ; Barroso, Joaquim Jose</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c328t-661f948f68b2fd3f72f1f97e0eccbd0e8a75f6f1abaad05d4f0dc9ce035626873</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Cavity resonators</topic><topic>characterization</topic><topic>Fabry-Perot cavity</topic><topic>Filled plastics</topic><topic>Holes</topic><topic>Lossless</topic><topic>Optical losses</topic><topic>Optical properties</topic><topic>Optical sensors</topic><topic>Physical properties</topic><topic>Porous silicon</topic><topic>Propagation losses</topic><topic>Reflectivity</topic><topic>Refractive index</topic><topic>Silicon</topic><topic>Substrates</topic><topic>transmittivity</topic><topic>Wavelengths</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hasar, Ugur C.</creatorcontrib><creatorcontrib>Ozbek, Ibrahim Y.</creatorcontrib><creatorcontrib>Cavusoglu, Bulent</creatorcontrib><creatorcontrib>Karacali, Tevhit</creatorcontrib><creatorcontrib>Efeoglu, Hasan</creatorcontrib><creatorcontrib>Ertugrul, Mehmet</creatorcontrib><creatorcontrib>Barroso, Joaquim Jose</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998–Present</collection><collection>IEEE Xplore</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><jtitle>IEEE journal of selected topics in quantum electronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Hasar, Ugur C.</au><au>Ozbek, Ibrahim Y.</au><au>Cavusoglu, Bulent</au><au>Karacali, Tevhit</au><au>Efeoglu, Hasan</au><au>Ertugrul, Mehmet</au><au>Barroso, Joaquim Jose</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Characterization of Porous Silicon Fabry-Pérot Optical Sensors for Reflectivity and Transmittivity Measurements</atitle><jtitle>IEEE journal of selected topics in quantum electronics</jtitle><stitle>JSTQE</stitle><date>2015-07</date><risdate>2015</risdate><volume>21</volume><issue>4</issue><spage>174</spage><epage>183</epage><pages>174-183</pages><issn>1077-260X</issn><eissn>1558-4542</eissn><coden>IJSQEN</coden><abstract>We investigate the effect of fabrication parameters (nonequal surface current densities, impurities inside the structure, etc.) and loss factor on reflectivity and transmittivity measurements from porous silicon Fabry-Pérot cavities with finite-size substrate thicknesses. We apply the formalism based on wave cascade matrix method for obtaining dependencies of reflectivity and transmittivity. From our analysis, we note the following results. First, resonance behavior of reflectivity and transmittivity changes only when optical/physical properties of middle layers of the cavity alter. Second, for lossless cavities, while reflectivity and transmittivity considerably change with surface characteristics (optical/physical properties of first layers), transmittivity is significantly modified by a change of optical/physical properties of middle layers (microcavity region). Third, loss inside a FP cavity makes the transmittivity more immune to variations in optical/physical properties of middle layers. Finally and most importantly, transmittivity values at resonance wavelength as well as the resonance wavelength shift can be utilized for the identification of unknown chemical/biological molecules by lossless FP cavities. For validation of these results, we carried out reflectivity and transmittivity measurements from some arbitrarily chosen positions but around the center of two fabricated FP cavities resonating at 1456 nm and at 542 nm.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/JSTQE.2014.2365583</doi><tpages>10</tpages></addata></record> |
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subjects | Cavity resonators characterization Fabry-Perot cavity Filled plastics Holes Lossless Optical losses Optical properties Optical sensors Physical properties Porous silicon Propagation losses Reflectivity Refractive index Silicon Substrates transmittivity Wavelengths |
title | Characterization of Porous Silicon Fabry-Pérot Optical Sensors for Reflectivity and Transmittivity Measurements |
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