Hydrogen evolution from a-C:H films
Diamond-like amorphous carbon films with high hardness, high electrical resistivity, good optical transparency into the infra-red, and good adherence to their substrates may be produced by many methods, most of which result in the incorporation of 20–40 at% hydrogen. These a-C:H films are similar to...
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Veröffentlicht in: | Vacuum 1985-01, Vol.35 (6), p.203-206 |
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description | Diamond-like amorphous carbon films with high hardness, high electrical resistivity, good optical transparency into the infra-red, and good adherence to their substrates may be produced by many methods, most of which result in the incorporation of 20–40 at% hydrogen. These a-C:H films are similar to a-Si:H films and the present work contributes additional evidence for this similarity. a-C:H films were deposited on glass or NaCl-coated glass in a capacitively coupled rf discharge in CH
4. The nature of the films depends upon the specific power density (SPD): polymeric for SPD < 10W cm
−2 torr
−1, diamond-like for SPD between 10 and 20, and graphitic for SPD>25. The amount of chemisorbed hydrogen in the films, as determined by differential scanned calorimetry (DSC), also depends on the SPD (and concomitant negative self-bias of the substrate), decreasing by a factor of six as the SPD increases from 10 to 20 and the negative self-bias increases form 400–650V. Additionally, the exothermic DSC peak sometimes consists of two or more partially resolved overlapping peaks. |
doi_str_mv | 10.1016/0042-207X(85)90390-2 |
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4. The nature of the films depends upon the specific power density (SPD): polymeric for SPD < 10W cm
−2 torr
−1, diamond-like for SPD between 10 and 20, and graphitic for SPD>25. The amount of chemisorbed hydrogen in the films, as determined by differential scanned calorimetry (DSC), also depends on the SPD (and concomitant negative self-bias of the substrate), decreasing by a factor of six as the SPD increases from 10 to 20 and the negative self-bias increases form 400–650V. Additionally, the exothermic DSC peak sometimes consists of two or more partially resolved overlapping peaks.</description><identifier>ISSN: 0042-207X</identifier><identifier>EISSN: 1879-2715</identifier><identifier>DOI: 10.1016/0042-207X(85)90390-2</identifier><identifier>CODEN: VACUAV</identifier><language>eng</language><publisher>Oxford: Elsevier Ltd</publisher><subject>Condensed matter: structure, mechanical and thermal properties ; Exact sciences and technology ; Physics ; Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties) ; Thin film structure and morphology</subject><ispartof>Vacuum, 1985-01, Vol.35 (6), p.203-206</ispartof><rights>1985</rights><rights>1986 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c313t-40596441d9fecca83a8de30a662bffa3a78271a19e236b03f8b3bdb90ba749113</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/0042207X85903902$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,776,780,3537,27901,27902,65534</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=8532645$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Nyaiesh, AR</creatorcontrib><creatorcontrib>Nowak, WB</creatorcontrib><title>Hydrogen evolution from a-C:H films</title><title>Vacuum</title><description>Diamond-like amorphous carbon films with high hardness, high electrical resistivity, good optical transparency into the infra-red, and good adherence to their substrates may be produced by many methods, most of which result in the incorporation of 20–40 at% hydrogen. These a-C:H films are similar to a-Si:H films and the present work contributes additional evidence for this similarity. a-C:H films were deposited on glass or NaCl-coated glass in a capacitively coupled rf discharge in CH
4. The nature of the films depends upon the specific power density (SPD): polymeric for SPD < 10W cm
−2 torr
−1, diamond-like for SPD between 10 and 20, and graphitic for SPD>25. The amount of chemisorbed hydrogen in the films, as determined by differential scanned calorimetry (DSC), also depends on the SPD (and concomitant negative self-bias of the substrate), decreasing by a factor of six as the SPD increases from 10 to 20 and the negative self-bias increases form 400–650V. Additionally, the exothermic DSC peak sometimes consists of two or more partially resolved overlapping peaks.</description><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Exact sciences and technology</subject><subject>Physics</subject><subject>Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties)</subject><subject>Thin film structure and morphology</subject><issn>0042-207X</issn><issn>1879-2715</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1985</creationdate><recordtype>article</recordtype><recordid>eNp9kE9LxDAUxIMouK5-Aw8FRfRQffnTNPEgyKKusOBFwVtI00QibbMm3YX99rbuskdP7_KbmTeD0DmGWwyY3wEwkhMoP69FcSOBSsjJAZpgUcqclLg4RJM9coxOUvoGAMJBTNDFfFPH8GW7zK5Ds-p96DIXQ5vpfHY_z5xv2nSKjpxukj3b3Sn6eH56n83zxdvL6-xxkRuKaZ8zKCRnDNfSWWO0oFrUloLmnFTOaapLMTyjsbSE8gqoExWt6kpCpUsmMaZTdLX1Xcbws7KpV61PxjaN7mxYJUVYITEvyQCyLWhiSClap5bRtzpuFAY1LqLGumqsq0Sh_hZRo-xy56-T0Y2LujM-7bWioISzYsAetpgduq69jSoZbztjax-t6VUd_P85vxYscqU</recordid><startdate>19850101</startdate><enddate>19850101</enddate><creator>Nyaiesh, AR</creator><creator>Nowak, WB</creator><general>Elsevier Ltd</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope></search><sort><creationdate>19850101</creationdate><title>Hydrogen evolution from a-C:H films</title><author>Nyaiesh, AR ; Nowak, WB</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c313t-40596441d9fecca83a8de30a662bffa3a78271a19e236b03f8b3bdb90ba749113</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1985</creationdate><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Exact sciences and technology</topic><topic>Physics</topic><topic>Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties)</topic><topic>Thin film structure and morphology</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Nyaiesh, AR</creatorcontrib><creatorcontrib>Nowak, WB</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><jtitle>Vacuum</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Nyaiesh, AR</au><au>Nowak, WB</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Hydrogen evolution from a-C:H films</atitle><jtitle>Vacuum</jtitle><date>1985-01-01</date><risdate>1985</risdate><volume>35</volume><issue>6</issue><spage>203</spage><epage>206</epage><pages>203-206</pages><issn>0042-207X</issn><eissn>1879-2715</eissn><coden>VACUAV</coden><abstract>Diamond-like amorphous carbon films with high hardness, high electrical resistivity, good optical transparency into the infra-red, and good adherence to their substrates may be produced by many methods, most of which result in the incorporation of 20–40 at% hydrogen. These a-C:H films are similar to a-Si:H films and the present work contributes additional evidence for this similarity. a-C:H films were deposited on glass or NaCl-coated glass in a capacitively coupled rf discharge in CH
4. The nature of the films depends upon the specific power density (SPD): polymeric for SPD < 10W cm
−2 torr
−1, diamond-like for SPD between 10 and 20, and graphitic for SPD>25. The amount of chemisorbed hydrogen in the films, as determined by differential scanned calorimetry (DSC), also depends on the SPD (and concomitant negative self-bias of the substrate), decreasing by a factor of six as the SPD increases from 10 to 20 and the negative self-bias increases form 400–650V. Additionally, the exothermic DSC peak sometimes consists of two or more partially resolved overlapping peaks.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/0042-207X(85)90390-2</doi><tpages>4</tpages></addata></record> |
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subjects | Condensed matter: structure, mechanical and thermal properties Exact sciences and technology Physics Surfaces and interfaces thin films and whiskers (structure and nonelectronic properties) Thin film structure and morphology |
title | Hydrogen evolution from a-C:H films |
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