Comparison of the structural properties of Zn-face and O-face single crystal homoepitaxial ZnO epilayers grown by RF-magnetron sputtering
Homoepitaxial ZnO growth is demonstrated from conventional RF-sputtering at 400 °C on both Zn and O polar faces of hydrothermally grown ZnO substrates. A minimum yield for the Rutherford backscattering and channeling spectrum, χmin , equal to ∼3% and ∼12% and a full width at half maximum of the 00.2...
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creator | Schifano, R. Riise, H. N. Domagala, J. Z. Azarov, A. Yu Ratajczak, R. Monakhov, E. V. Venkatachalapathy, V. Vines, L. Chan, K. S. Wong-Leung, J. Svensson, B. G. |
description | Homoepitaxial ZnO growth is demonstrated from conventional RF-sputtering at 400 °C on both Zn and O polar faces of hydrothermally grown ZnO substrates. A minimum yield for the Rutherford backscattering and channeling spectrum, χmin
, equal to ∼3% and ∼12% and a full width at half maximum of the 00.2 diffraction peak rocking curve of (70 ± 10) arc sec and (1400 ± 100) arc sec have been found for samples grown on the Zn and O face, respectively. The structural characteristics of the film deposited on the Zn face are comparable with those of epilayers grown by more complex techniques like molecular beam epitaxy. In contrast, the film simultaneously deposited on the O-face exhibits an inferior crystalline structure ∼0.7% strained in the c-direction and a higher atomic number contrast compared with the substrate, as revealed by high angle annular dark field imaging measurements. These differences between the Zn- and O-face films are discussed in detail and associated with the different growth mechanisms prevailing on the two surfaces. |
doi_str_mv | 10.1063/1.4973342 |
format | Article |
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, equal to ∼3% and ∼12% and a full width at half maximum of the 00.2 diffraction peak rocking curve of (70 ± 10) arc sec and (1400 ± 100) arc sec have been found for samples grown on the Zn and O face, respectively. The structural characteristics of the film deposited on the Zn face are comparable with those of epilayers grown by more complex techniques like molecular beam epitaxy. In contrast, the film simultaneously deposited on the O-face exhibits an inferior crystalline structure ∼0.7% strained in the c-direction and a higher atomic number contrast compared with the substrate, as revealed by high angle annular dark field imaging measurements. These differences between the Zn- and O-face films are discussed in detail and associated with the different growth mechanisms prevailing on the two surfaces.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.4973342</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Atomic properties ; Backscattering ; Channeling ; Crystal growth ; Crystal structure ; Epitaxial growth ; Magnetron sputtering ; Molecular beam epitaxy ; Single crystals ; Substrates ; Zinc oxide</subject><ispartof>Journal of applied physics, 2017-01, Vol.121 (1)</ispartof><rights>Author(s)</rights><rights>2017 Author(s). Published by AIP Publishing.</rights><rights>info:eu-repo/semantics/openAccess</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c452t-a569f08bf4bbf4beb13eb518e10308793d39d8a5af17ead6f0f29906aeb3aba93</citedby><cites>FETCH-LOGICAL-c452t-a569f08bf4bbf4beb13eb518e10308793d39d8a5af17ead6f0f29906aeb3aba93</cites><orcidid>0000-0003-0602-9624 ; 0000-0001-8684-2185 ; 0000-0002-6465-8851 ; 0000-0002-5050-4202 ; 0000-0001-8596-2230</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jap/article-lookup/doi/10.1063/1.4973342$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>230,314,776,780,790,881,4498,26544,27901,27902,76127</link.rule.ids></links><search><creatorcontrib>Schifano, R.</creatorcontrib><creatorcontrib>Riise, H. N.</creatorcontrib><creatorcontrib>Domagala, J. Z.</creatorcontrib><creatorcontrib>Azarov, A. Yu</creatorcontrib><creatorcontrib>Ratajczak, R.</creatorcontrib><creatorcontrib>Monakhov, E. V.</creatorcontrib><creatorcontrib>Venkatachalapathy, V.</creatorcontrib><creatorcontrib>Vines, L.</creatorcontrib><creatorcontrib>Chan, K. S.</creatorcontrib><creatorcontrib>Wong-Leung, J.</creatorcontrib><creatorcontrib>Svensson, B. G.</creatorcontrib><title>Comparison of the structural properties of Zn-face and O-face single crystal homoepitaxial ZnO epilayers grown by RF-magnetron sputtering</title><title>Journal of applied physics</title><description>Homoepitaxial ZnO growth is demonstrated from conventional RF-sputtering at 400 °C on both Zn and O polar faces of hydrothermally grown ZnO substrates. A minimum yield for the Rutherford backscattering and channeling spectrum, χmin
, equal to ∼3% and ∼12% and a full width at half maximum of the 00.2 diffraction peak rocking curve of (70 ± 10) arc sec and (1400 ± 100) arc sec have been found for samples grown on the Zn and O face, respectively. The structural characteristics of the film deposited on the Zn face are comparable with those of epilayers grown by more complex techniques like molecular beam epitaxy. In contrast, the film simultaneously deposited on the O-face exhibits an inferior crystalline structure ∼0.7% strained in the c-direction and a higher atomic number contrast compared with the substrate, as revealed by high angle annular dark field imaging measurements. These differences between the Zn- and O-face films are discussed in detail and associated with the different growth mechanisms prevailing on the two surfaces.</description><subject>Applied physics</subject><subject>Atomic properties</subject><subject>Backscattering</subject><subject>Channeling</subject><subject>Crystal growth</subject><subject>Crystal structure</subject><subject>Epitaxial growth</subject><subject>Magnetron sputtering</subject><subject>Molecular beam epitaxy</subject><subject>Single crystals</subject><subject>Substrates</subject><subject>Zinc oxide</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid>3HK</sourceid><recordid>eNp9kcFqGzEQQEVJoI6bQ7-ggpwSWFda7WpXx2DqNhAwlOTii5jdHdkbbGkjadv6E_rXkbHTHAo5DJpBjyfNDCGfOZtxJsVXPitUJUSRfyATzmqVVWXJzsiEsZxntarUR3IRwhNjnNdCTcjfudsN4PvgLHWGxg3SEP3YxtHDlg7eDehjj-FwubKZgRYp2I4uj2no7XqLtPX7EBO_cTuHQx_hT5-qlV3SVG1hjz7QtXe_LW329Oci28HaYvTpzTCMMaJPmk_k3MA24OXpnJLHxbeH-Y_sfvn9bn57n7VFmccMSqkMqxtTNIfAhgtsSl4jZ4LVlRKdUF0NJRheIXTSMJMrxSRgI6ABJabky9Hbpq5jb7V1HnSaVZlrKaSUibg6Eqn95xFD1E9u9DZ9Suc8L6QSSohEXb96XAgejR58vwO_Ty592IXm-rSLxN4c2dCm4cTe2X_wL-ffQD105j34f_MLWWqZTw</recordid><startdate>20170107</startdate><enddate>20170107</enddate><creator>Schifano, R.</creator><creator>Riise, H. 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G.</creator><general>American Institute of Physics</general><general>American Institute of Physics (AIP)</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>3HK</scope><orcidid>https://orcid.org/0000-0003-0602-9624</orcidid><orcidid>https://orcid.org/0000-0001-8684-2185</orcidid><orcidid>https://orcid.org/0000-0002-6465-8851</orcidid><orcidid>https://orcid.org/0000-0002-5050-4202</orcidid><orcidid>https://orcid.org/0000-0001-8596-2230</orcidid></search><sort><creationdate>20170107</creationdate><title>Comparison of the structural properties of Zn-face and O-face single crystal homoepitaxial ZnO epilayers grown by RF-magnetron sputtering</title><author>Schifano, R. ; Riise, H. N. ; Domagala, J. Z. ; Azarov, A. Yu ; Ratajczak, R. ; Monakhov, E. V. ; Venkatachalapathy, V. ; Vines, L. ; Chan, K. S. ; Wong-Leung, J. ; Svensson, B. 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G.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Comparison of the structural properties of Zn-face and O-face single crystal homoepitaxial ZnO epilayers grown by RF-magnetron sputtering</atitle><jtitle>Journal of applied physics</jtitle><date>2017-01-07</date><risdate>2017</risdate><volume>121</volume><issue>1</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>Homoepitaxial ZnO growth is demonstrated from conventional RF-sputtering at 400 °C on both Zn and O polar faces of hydrothermally grown ZnO substrates. A minimum yield for the Rutherford backscattering and channeling spectrum, χmin
, equal to ∼3% and ∼12% and a full width at half maximum of the 00.2 diffraction peak rocking curve of (70 ± 10) arc sec and (1400 ± 100) arc sec have been found for samples grown on the Zn and O face, respectively. The structural characteristics of the film deposited on the Zn face are comparable with those of epilayers grown by more complex techniques like molecular beam epitaxy. In contrast, the film simultaneously deposited on the O-face exhibits an inferior crystalline structure ∼0.7% strained in the c-direction and a higher atomic number contrast compared with the substrate, as revealed by high angle annular dark field imaging measurements. These differences between the Zn- and O-face films are discussed in detail and associated with the different growth mechanisms prevailing on the two surfaces.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4973342</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0003-0602-9624</orcidid><orcidid>https://orcid.org/0000-0001-8684-2185</orcidid><orcidid>https://orcid.org/0000-0002-6465-8851</orcidid><orcidid>https://orcid.org/0000-0002-5050-4202</orcidid><orcidid>https://orcid.org/0000-0001-8596-2230</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Applied physics Atomic properties Backscattering Channeling Crystal growth Crystal structure Epitaxial growth Magnetron sputtering Molecular beam epitaxy Single crystals Substrates Zinc oxide |
title | Comparison of the structural properties of Zn-face and O-face single crystal homoepitaxial ZnO epilayers grown by RF-magnetron sputtering |
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