Raman spectroscopy of chalcogenide thin films prepared by PLD
Chalcogenide glasses have many technological applications as a result of their particular optical and electrical properties. Ge–Se and Ag–Ge–Se systems were recently studied and tested as new materials for building non-volatile memories . Following these ideas, thin films of Ge–Se and Ag–Ge–Se were...
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Veröffentlicht in: | Journal of alloys and compounds 2010-04, Vol.495 (2), p.642-645 |
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creator | Erazú, M. Rocca, J. Fontana, M. Ureña, A. Arcondo, B. Pradel, A. |
description | Chalcogenide glasses have many technological applications as a result of their particular optical and electrical properties. Ge–Se and Ag–Ge–Se systems were recently studied and tested as new materials for building non-volatile memories
. Following these ideas, thin films of Ge–Se and Ag–Ge–Se were deposited using pulsed laser deposition (PLD). Ag was sputtered over binary films (for a composition between 0.05 and 0.25 Ag atomic fraction) and photo-diffused afterwards. Thus, three kinds of samples were analyzed by means of Raman spectroscopy, in order to provide information on the short- and medium-range order: PLD binary films before Ag doping, after Ag doping and PLD ternary films.
Before Ag doping, binary films exhibited Ge–Se corner-sharing tetrahedra modes at 190
cm
−1, low scattering from edge-sharing tetrahedra at 210
cm
−1, and Se chains at 260
cm
−1 (stretching mode). However, after the diffusion process was complete, we observed an intensity reduction of bands centered at 210
cm
−1 and 260
cm
−1. The spectra of the photo-diffused films were similar to those of films deposited using a ternary target. Relaxation effects in binary glasses were also analyzed. Results were compared with those of other authors. |
doi_str_mv | 10.1016/j.jallcom.2009.10.251 |
format | Article |
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. Following these ideas, thin films of Ge–Se and Ag–Ge–Se were deposited using pulsed laser deposition (PLD). Ag was sputtered over binary films (for a composition between 0.05 and 0.25 Ag atomic fraction) and photo-diffused afterwards. Thus, three kinds of samples were analyzed by means of Raman spectroscopy, in order to provide information on the short- and medium-range order: PLD binary films before Ag doping, after Ag doping and PLD ternary films.
Before Ag doping, binary films exhibited Ge–Se corner-sharing tetrahedra modes at 190
cm
−1, low scattering from edge-sharing tetrahedra at 210
cm
−1, and Se chains at 260
cm
−1 (stretching mode). However, after the diffusion process was complete, we observed an intensity reduction of bands centered at 210
cm
−1 and 260
cm
−1. The spectra of the photo-diffused films were similar to those of films deposited using a ternary target. Relaxation effects in binary glasses were also analyzed. Results were compared with those of other authors.</description><identifier>ISSN: 0925-8388</identifier><identifier>EISSN: 1873-4669</identifier><identifier>DOI: 10.1016/j.jallcom.2009.10.251</identifier><language>eng</language><publisher>Kidlington: Elsevier B.V</publisher><subject>Chalcogenides ; Chemical Sciences ; Condensed matter: structure, mechanical and thermal properties ; Cross-disciplinary physics: materials science; rheology ; Defects and impurities: doping, implantation, distribution, concentration, etc ; Deposition ; Doping ; Exact sciences and technology ; Glass ; Laser deposition ; Material chemistry ; Materials science ; Methods of deposition of films and coatings; film growth and epitaxy ; Physics ; Raman spectroscopy ; Silver ; Spectra ; Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties) ; Thin film structure and morphology ; Thin films</subject><ispartof>Journal of alloys and compounds, 2010-04, Vol.495 (2), p.642-645</ispartof><rights>2009 Elsevier B.V.</rights><rights>2015 INIST-CNRS</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c405t-943cb9d6ee3e65163111917557e4ad9f67aa513df38b5b3441e132fcc7e47223</citedby><cites>FETCH-LOGICAL-c405t-943cb9d6ee3e65163111917557e4ad9f67aa513df38b5b3441e132fcc7e47223</cites><orcidid>0000-0002-4588-8459</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.jallcom.2009.10.251$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>230,309,310,314,777,781,786,787,882,3537,23911,23912,25121,27905,27906,45976</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=22830402$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://hal.science/hal-00494203$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Erazú, M.</creatorcontrib><creatorcontrib>Rocca, J.</creatorcontrib><creatorcontrib>Fontana, M.</creatorcontrib><creatorcontrib>Ureña, A.</creatorcontrib><creatorcontrib>Arcondo, B.</creatorcontrib><creatorcontrib>Pradel, A.</creatorcontrib><title>Raman spectroscopy of chalcogenide thin films prepared by PLD</title><title>Journal of alloys and compounds</title><description>Chalcogenide glasses have many technological applications as a result of their particular optical and electrical properties. Ge–Se and Ag–Ge–Se systems were recently studied and tested as new materials for building non-volatile memories
. Following these ideas, thin films of Ge–Se and Ag–Ge–Se were deposited using pulsed laser deposition (PLD). Ag was sputtered over binary films (for a composition between 0.05 and 0.25 Ag atomic fraction) and photo-diffused afterwards. Thus, three kinds of samples were analyzed by means of Raman spectroscopy, in order to provide information on the short- and medium-range order: PLD binary films before Ag doping, after Ag doping and PLD ternary films.
Before Ag doping, binary films exhibited Ge–Se corner-sharing tetrahedra modes at 190
cm
−1, low scattering from edge-sharing tetrahedra at 210
cm
−1, and Se chains at 260
cm
−1 (stretching mode). However, after the diffusion process was complete, we observed an intensity reduction of bands centered at 210
cm
−1 and 260
cm
−1. The spectra of the photo-diffused films were similar to those of films deposited using a ternary target. Relaxation effects in binary glasses were also analyzed. Results were compared with those of other authors.</description><subject>Chalcogenides</subject><subject>Chemical Sciences</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Defects and impurities: doping, implantation, distribution, concentration, etc</subject><subject>Deposition</subject><subject>Doping</subject><subject>Exact sciences and technology</subject><subject>Glass</subject><subject>Laser deposition</subject><subject>Material chemistry</subject><subject>Materials science</subject><subject>Methods of deposition of films and coatings; film growth and epitaxy</subject><subject>Physics</subject><subject>Raman spectroscopy</subject><subject>Silver</subject><subject>Spectra</subject><subject>Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties)</subject><subject>Thin film structure and morphology</subject><subject>Thin films</subject><issn>0925-8388</issn><issn>1873-4669</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNqFkFtLAzEQhYMoWC8_QdgXER-2ZnLbzYOI1EuFgiK-hzQ7qyl7M2mF_nuztPjq08CZM2dmPkIugE6BgrpZTVe2aVzfThmlOmlTJuGATKAseC6U0odkQjWTecnL8picxLiilILmMCG377a1XRYHdOvQR9cP26yvM_dlU-Andr7CbP3lu6z2TRuzIeBgA1bZcpu9LR7OyFFtm4jn-3pKPp4eP2bzfPH6_DK7X-ROULnOteBuqSuFyFFJUBwANBRSFihspWtVWCuBVzUvl3LJhQAEzmrnUr9gjJ-S611susoMwbc2bE1vvZnfL8yoUSq0YJT_QPJe7bxD6L83GNem9dFh09gO-000pRK8VAx4csqd06XHY8D6LxqoGcGaldmDNSPYUU5g09zlfoONzjZ1sJ3z8W-YsZJTQcer73Y-TGR-PAYTncfOYeVDom2q3v-z6ReSiY7M</recordid><startdate>20100416</startdate><enddate>20100416</enddate><creator>Erazú, M.</creator><creator>Rocca, J.</creator><creator>Fontana, M.</creator><creator>Ureña, A.</creator><creator>Arcondo, B.</creator><creator>Pradel, A.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0002-4588-8459</orcidid></search><sort><creationdate>20100416</creationdate><title>Raman spectroscopy of chalcogenide thin films prepared by PLD</title><author>Erazú, M. ; Rocca, J. ; Fontana, M. ; Ureña, A. ; Arcondo, B. ; Pradel, A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c405t-943cb9d6ee3e65163111917557e4ad9f67aa513df38b5b3441e132fcc7e47223</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>Chalcogenides</topic><topic>Chemical Sciences</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Defects and impurities: doping, implantation, distribution, concentration, etc</topic><topic>Deposition</topic><topic>Doping</topic><topic>Exact sciences and technology</topic><topic>Glass</topic><topic>Laser deposition</topic><topic>Material chemistry</topic><topic>Materials science</topic><topic>Methods of deposition of films and coatings; film growth and epitaxy</topic><topic>Physics</topic><topic>Raman spectroscopy</topic><topic>Silver</topic><topic>Spectra</topic><topic>Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties)</topic><topic>Thin film structure and morphology</topic><topic>Thin films</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Erazú, M.</creatorcontrib><creatorcontrib>Rocca, J.</creatorcontrib><creatorcontrib>Fontana, M.</creatorcontrib><creatorcontrib>Ureña, A.</creatorcontrib><creatorcontrib>Arcondo, B.</creatorcontrib><creatorcontrib>Pradel, A.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Journal of alloys and compounds</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Erazú, M.</au><au>Rocca, J.</au><au>Fontana, M.</au><au>Ureña, A.</au><au>Arcondo, B.</au><au>Pradel, A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Raman spectroscopy of chalcogenide thin films prepared by PLD</atitle><jtitle>Journal of alloys and compounds</jtitle><date>2010-04-16</date><risdate>2010</risdate><volume>495</volume><issue>2</issue><spage>642</spage><epage>645</epage><pages>642-645</pages><issn>0925-8388</issn><eissn>1873-4669</eissn><abstract>Chalcogenide glasses have many technological applications as a result of their particular optical and electrical properties. Ge–Se and Ag–Ge–Se systems were recently studied and tested as new materials for building non-volatile memories
. Following these ideas, thin films of Ge–Se and Ag–Ge–Se were deposited using pulsed laser deposition (PLD). Ag was sputtered over binary films (for a composition between 0.05 and 0.25 Ag atomic fraction) and photo-diffused afterwards. Thus, three kinds of samples were analyzed by means of Raman spectroscopy, in order to provide information on the short- and medium-range order: PLD binary films before Ag doping, after Ag doping and PLD ternary films.
Before Ag doping, binary films exhibited Ge–Se corner-sharing tetrahedra modes at 190
cm
−1, low scattering from edge-sharing tetrahedra at 210
cm
−1, and Se chains at 260
cm
−1 (stretching mode). However, after the diffusion process was complete, we observed an intensity reduction of bands centered at 210
cm
−1 and 260
cm
−1. The spectra of the photo-diffused films were similar to those of films deposited using a ternary target. Relaxation effects in binary glasses were also analyzed. Results were compared with those of other authors.</abstract><cop>Kidlington</cop><pub>Elsevier B.V</pub><doi>10.1016/j.jallcom.2009.10.251</doi><tpages>4</tpages><orcidid>https://orcid.org/0000-0002-4588-8459</orcidid></addata></record> |
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subjects | Chalcogenides Chemical Sciences Condensed matter: structure, mechanical and thermal properties Cross-disciplinary physics: materials science rheology Defects and impurities: doping, implantation, distribution, concentration, etc Deposition Doping Exact sciences and technology Glass Laser deposition Material chemistry Materials science Methods of deposition of films and coatings film growth and epitaxy Physics Raman spectroscopy Silver Spectra Surfaces and interfaces thin films and whiskers (structure and nonelectronic properties) Thin film structure and morphology Thin films |
title | Raman spectroscopy of chalcogenide thin films prepared by PLD |
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