Interference-enhanced Raman scattering of F sub(16)CuPc thin films
Interference-enhanced Raman scattering (IERS) was observed for thin films of copper(II) hexadecafluorophthalocyanine (F sub(16)CuPc) deposited on SiO sub(2) layers on a Si substrate. The enhancement of the Raman scattering originates from the interference of the light in the transparent SiO sub(2) l...
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Veröffentlicht in: | Journal of physics. D, Applied physics Applied physics, 2016-03, Vol.49 (11), p.115502-115508 |
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creator | Solonenko, D Gordan, O D Milekhin, A Panholzer, M Hingerl, K Zahn, D R T |
description | Interference-enhanced Raman scattering (IERS) was observed for thin films of copper(II) hexadecafluorophthalocyanine (F sub(16)CuPc) deposited on SiO sub(2) layers on a Si substrate. The enhancement of the Raman scattering originates from the interference of the light in the transparent SiO sub(2) layer. Stripes of SiO sub(2)/Si with gradually varying oxide layer thickness were used as IERS substrates for a systematic study of the enhancement parameters. Raman measurements were carried out using three laser lines (325, 514.7, and 632.8 nm) in order to probe the F sub(16)CuPc thin films at non-resonant and resonant Raman conditions. Spectroscopic ellipsometry was used to determine both the SiO sub(2) layer and thin film thicknesses. The intensity enhancement of the F sub(16)CuPc Raman peaks occurs periodically, corresponding to the alternating interference conditions for the Raman scattered light with increasing SiO sub(2) layer thickness. The enhancement factors were calculated using the optical constants of the layers involved and the geometric parameters. This allows a straightforward application of IERS for optical studies of thin films and interfaces by calculating the dielectric thickness where maximum Raman enhancement is expected. |
doi_str_mv | 10.1088/0022-3727/49/11/115502 |
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The enhancement of the Raman scattering originates from the interference of the light in the transparent SiO sub(2) layer. Stripes of SiO sub(2)/Si with gradually varying oxide layer thickness were used as IERS substrates for a systematic study of the enhancement parameters. Raman measurements were carried out using three laser lines (325, 514.7, and 632.8 nm) in order to probe the F sub(16)CuPc thin films at non-resonant and resonant Raman conditions. Spectroscopic ellipsometry was used to determine both the SiO sub(2) layer and thin film thicknesses. The intensity enhancement of the F sub(16)CuPc Raman peaks occurs periodically, corresponding to the alternating interference conditions for the Raman scattered light with increasing SiO sub(2) layer thickness. The enhancement factors were calculated using the optical constants of the layers involved and the geometric parameters. This allows a straightforward application of IERS for optical studies of thin films and interfaces by calculating the dielectric thickness where maximum Raman enhancement is expected.</description><identifier>ISSN: 0022-3727</identifier><identifier>EISSN: 1361-6463</identifier><identifier>DOI: 10.1088/0022-3727/49/11/115502</identifier><language>eng</language><subject>Interference ; Mathematical analysis ; Oxides ; Raman scattering ; Silicon dioxide ; Silicon substrates ; Thickness ; Thin films</subject><ispartof>Journal of physics. 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The enhancement of the Raman scattering originates from the interference of the light in the transparent SiO sub(2) layer. Stripes of SiO sub(2)/Si with gradually varying oxide layer thickness were used as IERS substrates for a systematic study of the enhancement parameters. Raman measurements were carried out using three laser lines (325, 514.7, and 632.8 nm) in order to probe the F sub(16)CuPc thin films at non-resonant and resonant Raman conditions. Spectroscopic ellipsometry was used to determine both the SiO sub(2) layer and thin film thicknesses. The intensity enhancement of the F sub(16)CuPc Raman peaks occurs periodically, corresponding to the alternating interference conditions for the Raman scattered light with increasing SiO sub(2) layer thickness. The enhancement factors were calculated using the optical constants of the layers involved and the geometric parameters. This allows a straightforward application of IERS for optical studies of thin films and interfaces by calculating the dielectric thickness where maximum Raman enhancement is expected.</description><subject>Interference</subject><subject>Mathematical analysis</subject><subject>Oxides</subject><subject>Raman scattering</subject><subject>Silicon dioxide</subject><subject>Silicon substrates</subject><subject>Thickness</subject><subject>Thin films</subject><issn>0022-3727</issn><issn>1361-6463</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqVisGuwUAUQCfyJPrwCzJLFtV7ZzqjtoSwE7GXUbdU2im97f_rQuwlJzmLc4SYIMwRkiQCUCrUC7WI4mWE2GEMqJ4IUFsMbWz1nwi-00D8Mz8AwNgEA7Ha-4bqjGryKYXk767zVR5d6bzk1DVdzf1NVpncSm4vU7SzdXtIZXPPvczyouSR6GeuYBp_PBTT7ea03oXPunq1xM25zDmlonCeqpbPmCgTG4i11T-sb_GxQ_M</recordid><startdate>20160301</startdate><enddate>20160301</enddate><creator>Solonenko, D</creator><creator>Gordan, O D</creator><creator>Milekhin, A</creator><creator>Panholzer, M</creator><creator>Hingerl, K</creator><creator>Zahn, D R T</creator><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope></search><sort><creationdate>20160301</creationdate><title>Interference-enhanced Raman scattering of F sub(16)CuPc thin films</title><author>Solonenko, D ; Gordan, O D ; Milekhin, A ; Panholzer, M ; Hingerl, K ; Zahn, D R T</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_miscellaneous_18254504363</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Interference</topic><topic>Mathematical analysis</topic><topic>Oxides</topic><topic>Raman scattering</topic><topic>Silicon dioxide</topic><topic>Silicon substrates</topic><topic>Thickness</topic><topic>Thin films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Solonenko, D</creatorcontrib><creatorcontrib>Gordan, O D</creatorcontrib><creatorcontrib>Milekhin, A</creatorcontrib><creatorcontrib>Panholzer, M</creatorcontrib><creatorcontrib>Hingerl, K</creatorcontrib><creatorcontrib>Zahn, D R T</creatorcontrib><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 physics. D, Applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Solonenko, D</au><au>Gordan, O D</au><au>Milekhin, A</au><au>Panholzer, M</au><au>Hingerl, K</au><au>Zahn, D R T</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Interference-enhanced Raman scattering of F sub(16)CuPc thin films</atitle><jtitle>Journal of physics. D, Applied physics</jtitle><date>2016-03-01</date><risdate>2016</risdate><volume>49</volume><issue>11</issue><spage>115502</spage><epage>115508</epage><pages>115502-115508</pages><issn>0022-3727</issn><eissn>1361-6463</eissn><abstract>Interference-enhanced Raman scattering (IERS) was observed for thin films of copper(II) hexadecafluorophthalocyanine (F sub(16)CuPc) deposited on SiO sub(2) layers on a Si substrate. The enhancement of the Raman scattering originates from the interference of the light in the transparent SiO sub(2) layer. Stripes of SiO sub(2)/Si with gradually varying oxide layer thickness were used as IERS substrates for a systematic study of the enhancement parameters. Raman measurements were carried out using three laser lines (325, 514.7, and 632.8 nm) in order to probe the F sub(16)CuPc thin films at non-resonant and resonant Raman conditions. Spectroscopic ellipsometry was used to determine both the SiO sub(2) layer and thin film thicknesses. The intensity enhancement of the F sub(16)CuPc Raman peaks occurs periodically, corresponding to the alternating interference conditions for the Raman scattered light with increasing SiO sub(2) layer thickness. The enhancement factors were calculated using the optical constants of the layers involved and the geometric parameters. This allows a straightforward application of IERS for optical studies of thin films and interfaces by calculating the dielectric thickness where maximum Raman enhancement is expected.</abstract><doi>10.1088/0022-3727/49/11/115502</doi></addata></record> |
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subjects | Interference Mathematical analysis Oxides Raman scattering Silicon dioxide Silicon substrates Thickness Thin films |
title | Interference-enhanced Raman scattering of F sub(16)CuPc thin films |
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