Epitaxial growth of Si1−xGex alloys and Ge on Si(100) by electron-cyclotron-resonance Ar plasma chemical vapor deposition without substrate heating
By using electron-cyclotron-resonance (ECR) Ar-plasma chemical vapor deposition (CVD) without substrate heating, the epitaxial growth process of Si1−xGex alloy and Ge films deposited directly on dilute-HF-treated Si(100) was investigated. From the reflection high energy electron diffraction patterns...
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description | By using electron-cyclotron-resonance (ECR) Ar-plasma chemical vapor deposition (CVD) without substrate heating, the epitaxial growth process of Si1−xGex alloy and Ge films deposited directly on dilute-HF-treated Si(100) was investigated. From the reflection high energy electron diffraction patterns of the deposited Si1−xGex alloy (x=0.50, 0.75) and Ge films on Si(100), it is confirmed that epitaxial growth can be realized without substrate heating, and that crystallinity degradation at larger film thickness is observed. The X-ray diffraction peak of the epitaxial films reveals the existence of large compressive strain, which is induced by lattice matching with the Si(100) substrate at smaller film thicknesses, as well as strain relaxation behavior at larger film thicknesses. The Ge fraction of Si1−xGex thin film is in good agreement with the normalized GeH4 partial pressure. The Si1−xGex deposition rate increases with an increase of GeH4 partial pressure. The GeH4 partial pressure dependence of partial deposition rates [(Si or Ge fraction)×(Si1−xGex thickness)/(deposition time)] shows that the Si partial deposition rate is slightly enhanced by the existence of Ge. From these results, it is proposed that the ECR-plasma CVD process can be utilized for Ge fraction control in highly-strained heterostructure formation of group IV semiconductors.
•Si1−xGex alloy and Ge were epitaxially grown on Si(100) without substrate heating.•Large strain and its relaxation behavior can be observed by X-ray diffraction.•Ge fraction of Si1−xGex is equal to normalized GeH4 partial pressure.•Si partial deposition rate is slightly enhanced by existence of Ge. |
doi_str_mv | 10.1016/j.tsf.2013.11.023 |
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•Si1−xGex alloy and Ge were epitaxially grown on Si(100) without substrate heating.•Large strain and its relaxation behavior can be observed by X-ray diffraction.•Ge fraction of Si1−xGex is equal to normalized GeH4 partial pressure.•Si partial deposition rate is slightly enhanced by existence of Ge.</description><identifier>ISSN: 0040-6090</identifier><identifier>EISSN: 1879-2731</identifier><identifier>DOI: 10.1016/j.tsf.2013.11.023</identifier><identifier>CODEN: THSFAP</identifier><language>eng</language><publisher>Amsterdam: Elsevier B.V</publisher><subject>Chemical vapor deposition ; Chemical vapor deposition (including plasma-enhanced cvd, mocvd, etc.) ; Cross-disciplinary physics: materials science; rheology ; Deposition ; Epitaxial growth ; Exact sciences and technology ; Film thickness ; Germanium ; Heating ; Heterostructure ; Ion and electron beam-assisted deposition; ion plating ; Materials science ; Methods of deposition of films and coatings; film growth and epitaxy ; Partial pressure ; Physics ; Physics of gases, plasmas and electric discharges ; Physics of plasmas and electric discharges ; Plasma applications ; Plasma chemical vapor deposition ; Plasma-based ion implantation and deposition ; Raman scattering spectroscopy ; Semiconductors ; Silicon ; Silicon–germanium alloy ; Substrates ; Theory and models of film growth ; X-ray diffraction</subject><ispartof>Thin solid films, 2014-04, Vol.557, p.31-35</ispartof><rights>2013 Elsevier B.V.</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c341t-8e0cfc9b320445132ca4a3e9a582bdef9a9c82e3f545a527d7a356c13b2bc10f3</citedby><cites>FETCH-LOGICAL-c341t-8e0cfc9b320445132ca4a3e9a582bdef9a9c82e3f545a527d7a356c13b2bc10f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.tsf.2013.11.023$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>310,311,315,781,785,790,791,3551,23932,23933,25142,27926,27927,45997</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=28423450$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Ueno, Naofumi</creatorcontrib><creatorcontrib>Sakuraba, Masao</creatorcontrib><creatorcontrib>Murota, Junichi</creatorcontrib><creatorcontrib>Sato, Shigeo</creatorcontrib><title>Epitaxial growth of Si1−xGex alloys and Ge on Si(100) by electron-cyclotron-resonance Ar plasma chemical vapor deposition without substrate heating</title><title>Thin solid films</title><description>By using electron-cyclotron-resonance (ECR) Ar-plasma chemical vapor deposition (CVD) without substrate heating, the epitaxial growth process of Si1−xGex alloy and Ge films deposited directly on dilute-HF-treated Si(100) was investigated. From the reflection high energy electron diffraction patterns of the deposited Si1−xGex alloy (x=0.50, 0.75) and Ge films on Si(100), it is confirmed that epitaxial growth can be realized without substrate heating, and that crystallinity degradation at larger film thickness is observed. The X-ray diffraction peak of the epitaxial films reveals the existence of large compressive strain, which is induced by lattice matching with the Si(100) substrate at smaller film thicknesses, as well as strain relaxation behavior at larger film thicknesses. The Ge fraction of Si1−xGex thin film is in good agreement with the normalized GeH4 partial pressure. The Si1−xGex deposition rate increases with an increase of GeH4 partial pressure. The GeH4 partial pressure dependence of partial deposition rates [(Si or Ge fraction)×(Si1−xGex thickness)/(deposition time)] shows that the Si partial deposition rate is slightly enhanced by the existence of Ge. From these results, it is proposed that the ECR-plasma CVD process can be utilized for Ge fraction control in highly-strained heterostructure formation of group IV semiconductors.
•Si1−xGex alloy and Ge were epitaxially grown on Si(100) without substrate heating.•Large strain and its relaxation behavior can be observed by X-ray diffraction.•Ge fraction of Si1−xGex is equal to normalized GeH4 partial pressure.•Si partial deposition rate is slightly enhanced by existence of Ge.</description><subject>Chemical vapor deposition</subject><subject>Chemical vapor deposition (including plasma-enhanced cvd, mocvd, etc.)</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Deposition</subject><subject>Epitaxial growth</subject><subject>Exact sciences and technology</subject><subject>Film thickness</subject><subject>Germanium</subject><subject>Heating</subject><subject>Heterostructure</subject><subject>Ion and electron beam-assisted deposition; ion plating</subject><subject>Materials science</subject><subject>Methods of deposition of films and coatings; film growth and epitaxy</subject><subject>Partial pressure</subject><subject>Physics</subject><subject>Physics of gases, plasmas and electric discharges</subject><subject>Physics of plasmas and electric discharges</subject><subject>Plasma applications</subject><subject>Plasma chemical vapor deposition</subject><subject>Plasma-based ion implantation and deposition</subject><subject>Raman scattering spectroscopy</subject><subject>Semiconductors</subject><subject>Silicon</subject><subject>Silicon–germanium alloy</subject><subject>Substrates</subject><subject>Theory and models of film growth</subject><subject>X-ray diffraction</subject><issn>0040-6090</issn><issn>1879-2731</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNp9kcFu1DAQhiMEEkvLA3DzBakcEmbsZJOIU1WVbaVKHApna-JMul5l42B729034IzEC_IkeNmKI76MpfnnH833Z9k7hAIBlx83RQxDIQFVgViAVC-yBTZ1m8ta4ctsAVBCvoQWXmdvQtgAAEqpFtmv69lG2lsaxYN3T3Et3CDuLf7-8XO_4r2gcXSHIGjqxYqFm1LvAgE-iO4geGQTvZtyczCj-_vzHNxEk2Fx6cU8UtiSMGveWpMWPNLsvOh5dsFGm7yebFy7XRRh14XoKbJYM0U7PZxnrwYaA799rmfZt8_XX69u8rsvq9ury7vcqBJj3jCYwbSdklCWFSppqCTFLVWN7HoeWmpNI1kNVVlRJeu-JlUtDapOdgZhUGfZxcl39u77jkPUWxsMjyNN7HZBHwmm19RlkuJJarwLwfOgZ2-35A8aQR8j0BudItDHCDSiThGkmffP9hQSgMEnMjb8G5RNKVVZQdJ9Ouk43fpo2etgLCeKvfUJse6d_c-WP_8Jntw</recordid><startdate>20140401</startdate><enddate>20140401</enddate><creator>Ueno, Naofumi</creator><creator>Sakuraba, Masao</creator><creator>Murota, Junichi</creator><creator>Sato, Shigeo</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20140401</creationdate><title>Epitaxial growth of Si1−xGex alloys and Ge on Si(100) by electron-cyclotron-resonance Ar plasma chemical vapor deposition without substrate heating</title><author>Ueno, Naofumi ; Sakuraba, Masao ; Murota, Junichi ; Sato, Shigeo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c341t-8e0cfc9b320445132ca4a3e9a582bdef9a9c82e3f545a527d7a356c13b2bc10f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Chemical vapor deposition</topic><topic>Chemical vapor deposition (including plasma-enhanced cvd, mocvd, etc.)</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Deposition</topic><topic>Epitaxial growth</topic><topic>Exact sciences and technology</topic><topic>Film thickness</topic><topic>Germanium</topic><topic>Heating</topic><topic>Heterostructure</topic><topic>Ion and electron beam-assisted deposition; ion plating</topic><topic>Materials science</topic><topic>Methods of deposition of films and coatings; film growth and epitaxy</topic><topic>Partial pressure</topic><topic>Physics</topic><topic>Physics of gases, plasmas and electric discharges</topic><topic>Physics of plasmas and electric discharges</topic><topic>Plasma applications</topic><topic>Plasma chemical vapor deposition</topic><topic>Plasma-based ion implantation and deposition</topic><topic>Raman scattering spectroscopy</topic><topic>Semiconductors</topic><topic>Silicon</topic><topic>Silicon–germanium alloy</topic><topic>Substrates</topic><topic>Theory and models of film growth</topic><topic>X-ray diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ueno, Naofumi</creatorcontrib><creatorcontrib>Sakuraba, Masao</creatorcontrib><creatorcontrib>Murota, Junichi</creatorcontrib><creatorcontrib>Sato, Shigeo</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Thin solid films</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ueno, Naofumi</au><au>Sakuraba, Masao</au><au>Murota, Junichi</au><au>Sato, Shigeo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Epitaxial growth of Si1−xGex alloys and Ge on Si(100) by electron-cyclotron-resonance Ar plasma chemical vapor deposition without substrate heating</atitle><jtitle>Thin solid films</jtitle><date>2014-04-01</date><risdate>2014</risdate><volume>557</volume><spage>31</spage><epage>35</epage><pages>31-35</pages><issn>0040-6090</issn><eissn>1879-2731</eissn><coden>THSFAP</coden><abstract>By using electron-cyclotron-resonance (ECR) Ar-plasma chemical vapor deposition (CVD) without substrate heating, the epitaxial growth process of Si1−xGex alloy and Ge films deposited directly on dilute-HF-treated Si(100) was investigated. From the reflection high energy electron diffraction patterns of the deposited Si1−xGex alloy (x=0.50, 0.75) and Ge films on Si(100), it is confirmed that epitaxial growth can be realized without substrate heating, and that crystallinity degradation at larger film thickness is observed. The X-ray diffraction peak of the epitaxial films reveals the existence of large compressive strain, which is induced by lattice matching with the Si(100) substrate at smaller film thicknesses, as well as strain relaxation behavior at larger film thicknesses. The Ge fraction of Si1−xGex thin film is in good agreement with the normalized GeH4 partial pressure. The Si1−xGex deposition rate increases with an increase of GeH4 partial pressure. The GeH4 partial pressure dependence of partial deposition rates [(Si or Ge fraction)×(Si1−xGex thickness)/(deposition time)] shows that the Si partial deposition rate is slightly enhanced by the existence of Ge. From these results, it is proposed that the ECR-plasma CVD process can be utilized for Ge fraction control in highly-strained heterostructure formation of group IV semiconductors.
•Si1−xGex alloy and Ge were epitaxially grown on Si(100) without substrate heating.•Large strain and its relaxation behavior can be observed by X-ray diffraction.•Ge fraction of Si1−xGex is equal to normalized GeH4 partial pressure.•Si partial deposition rate is slightly enhanced by existence of Ge.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.tsf.2013.11.023</doi><tpages>5</tpages></addata></record> |
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subjects | Chemical vapor deposition Chemical vapor deposition (including plasma-enhanced cvd, mocvd, etc.) Cross-disciplinary physics: materials science rheology Deposition Epitaxial growth Exact sciences and technology Film thickness Germanium Heating Heterostructure Ion and electron beam-assisted deposition ion plating Materials science Methods of deposition of films and coatings film growth and epitaxy Partial pressure Physics Physics of gases, plasmas and electric discharges Physics of plasmas and electric discharges Plasma applications Plasma chemical vapor deposition Plasma-based ion implantation and deposition Raman scattering spectroscopy Semiconductors Silicon Silicon–germanium alloy Substrates Theory and models of film growth X-ray diffraction |
title | Epitaxial growth of Si1−xGex alloys and Ge on Si(100) by electron-cyclotron-resonance Ar plasma chemical vapor deposition without substrate heating |
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