Thickness optimization of Mo films for Cu(InGa)Se2 solar cell applications
Mo thin films are deposited on soda lime glass (SLG) substrates using DC magnetron sputtering. The Mo film thicknesses are varied from 0.08 Delta *mm to 1.5 Delta *mm to gain a better understanding of the growth process of the film. The residual stresses and the structural properties of these films...
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Veröffentlicht in: | Chinese physics B 2011-06, Vol.20 (6), p.068102-jQuery1323923676442='49' |
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creator | Li, Wei (微李) Zhao, Yan-Min (彦民 赵) Liu, Xing-Jiang (兴江 刘) Ao, Jian-Ping (建平 敖) Sun, Yun (云孙) |
description | Mo thin films are deposited on soda lime glass (SLG) substrates using DC magnetron sputtering. The Mo film thicknesses are varied from 0.08 Delta *mm to 1.5 Delta *mm to gain a better understanding of the growth process of the film. The residual stresses and the structural properties of these films are investigated, with attention paid particularly to the film thickness dependence of these properties. Residual stress decreases and yields a typical tensile-to-compressive stress transition with the increase of film thickness at the first stages of film growth. The stress tends to be stable with the further increase of film thickness. Using the Mo film with an optimum thickness of 1 Delta *mm as the back contact, the Cu(InGa)Se2 solar cell can reach a conversion efficiency of 13.15%. |
doi_str_mv | 10.1088/1674-1056/20/6/068102 |
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The Mo film thicknesses are varied from 0.08 Delta *mm to 1.5 Delta *mm to gain a better understanding of the growth process of the film. The residual stresses and the structural properties of these films are investigated, with attention paid particularly to the film thickness dependence of these properties. Residual stress decreases and yields a typical tensile-to-compressive stress transition with the increase of film thickness at the first stages of film growth. The stress tends to be stable with the further increase of film thickness. Using the Mo film with an optimum thickness of 1 Delta *mm as the back contact, the Cu(InGa)Se2 solar cell can reach a conversion efficiency of 13.15%.</description><subject>APPLICATIONS</subject><subject>COPPER INDIUM SELENIDE</subject><subject>COPPER SELENIDE</subject><subject>DEPOSITION</subject><subject>Film growth</subject><subject>Film thickness</subject><subject>Optimization</subject><subject>Photovoltaic cells</subject><subject>RESIDUAL STRESS</subject><subject>SOLAR CELLS</subject><subject>STRESS</subject><subject>Stresses</subject><subject>THIN FILMS</subject><issn>1674-1056</issn><issn>2058-3834</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNqFkLFOwzAQhi0EEqXwCEgei0TI2U7tZEQVLUVFDJTZchJbGJLYxOkAT49DEVMlbrnhvv_u9CF0SeCGQJ6nhIssITDnKYWUp8BzAvQITSjM84TlLDtGkz_mFJ2F8AbAI8Mm6GH7aqv3ToeAnR9sa7_UYF2HncGPDhvbtAEb1-PFbrbuVurqWVMcXKN6XOmmwcr7xlY_kXCOToxqgr747VP0srzbLu6TzdNqvbjdJJaSbEhKClwolemaFlyQoq51zoGVrNSxalEYPa8FkDgFzhmUBaEVVUSYLDMF42yKZvu9vncfOx0G2dowfqM67XZBEiHy6IBT8T8KUWC8w2hEYY9a56Xvbav6zziXo2E52pOjPUlBcrk3HCPXByKHUOlrw74Bzcl5-A</recordid><startdate>20110601</startdate><enddate>20110601</enddate><creator>Li, Wei (微李)</creator><creator>Zhao, Yan-Min (彦民 赵)</creator><creator>Liu, Xing-Jiang (兴江 刘)</creator><creator>Ao, Jian-Ping (建平 敖)</creator><creator>Sun, Yun (云孙)</creator><general>IOP Publishing</general><scope>7U5</scope><scope>8FD</scope><scope>H8G</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20110601</creationdate><title>Thickness optimization of Mo films for Cu(InGa)Se2 solar cell applications</title><author>Li, Wei (微李) ; Zhao, Yan-Min (彦民 赵) ; Liu, Xing-Jiang (兴江 刘) ; Ao, Jian-Ping (建平 敖) ; Sun, Yun (云孙)</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i214t-b2067aa4ed296719dde8603b3beeeed79fe5d70129606630b912c2a17f44f9363</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>APPLICATIONS</topic><topic>COPPER INDIUM SELENIDE</topic><topic>COPPER SELENIDE</topic><topic>DEPOSITION</topic><topic>Film growth</topic><topic>Film thickness</topic><topic>Optimization</topic><topic>Photovoltaic cells</topic><topic>RESIDUAL STRESS</topic><topic>SOLAR CELLS</topic><topic>STRESS</topic><topic>Stresses</topic><topic>THIN FILMS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Li, Wei (微李)</creatorcontrib><creatorcontrib>Zhao, Yan-Min (彦民 赵)</creatorcontrib><creatorcontrib>Liu, Xing-Jiang (兴江 刘)</creatorcontrib><creatorcontrib>Ao, Jian-Ping (建平 敖)</creatorcontrib><creatorcontrib>Sun, Yun (云孙)</creatorcontrib><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Copper Technical Reference Library</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Chinese physics B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Li, Wei (微李)</au><au>Zhao, Yan-Min (彦民 赵)</au><au>Liu, Xing-Jiang (兴江 刘)</au><au>Ao, Jian-Ping (建平 敖)</au><au>Sun, Yun (云孙)</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Thickness optimization of Mo films for Cu(InGa)Se2 solar cell applications</atitle><jtitle>Chinese physics B</jtitle><date>2011-06-01</date><risdate>2011</risdate><volume>20</volume><issue>6</issue><spage>068102</spage><epage>jQuery1323923676442='49'</epage><pages>068102-jQuery1323923676442='49'</pages><issn>1674-1056</issn><eissn>2058-3834</eissn><abstract>Mo thin films are deposited on soda lime glass (SLG) substrates using DC magnetron sputtering. 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subjects | APPLICATIONS COPPER INDIUM SELENIDE COPPER SELENIDE DEPOSITION Film growth Film thickness Optimization Photovoltaic cells RESIDUAL STRESS SOLAR CELLS STRESS Stresses THIN FILMS |
title | Thickness optimization of Mo films for Cu(InGa)Se2 solar cell applications |
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