Si surface orientation dependence of SiC-dot formation in bulk-Si using hot-C+-ion implantation technique
We experimentally investigated the Si surface orientation dependence of SiC-dot formation and photoluminescence (PL) properties in three (100)-, (110)-, and (111)-bulk-Si substrates (C+–Si) with different surface densities of Si atoms (NS), where SiC-dots were fabricated by a hot-C+ ion implantation...
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description | We experimentally investigated the Si surface orientation dependence of SiC-dot formation and photoluminescence (PL) properties in three (100)-, (110)-, and (111)-bulk-Si substrates (C+–Si) with different surface densities of Si atoms (NS), where SiC-dots were fabricated by a hot-C+ ion implantation into bulk-Si and post-N2 annealing processes. Transmission electron microscopy observation and x-ray photoelectron spectroscopy revealed the formation of SiC-dots in the (110)- and (111)-C+–Si, in addition to (100)-C+–Si. The diameter (Φ) and surface density (ND) of the SiC-dots depended on the Si surface orientation, and the average Φ of the SiC-dots in three surface-oriented C+–Si decreased from approximately 5–3 nm with increasing NS because the trapping value of C-ions at SiO2/Si interface increased with increasing NS, which leads to the reduction of C-ions to convert SiC-dots in the SiC-dot formation area under higher NS condition. However, the UV-Raman intensity of the TO mode of Si−C vibration was nearly independent of NS. We experimentally confirmed the PL emissions from the (110)- and (111)-C+–Si in addition to the (100)-C+–Si. As a result, the PL spectrum and PL emission coefficient (η) of the SiC-dots strongly depended on the Si surface orientation. The PL intensity IPL of the SiC-dots strongly depended on the NS because the η of the SiC-dots significantly increased with decreasing Φ, although SiC-dots in Si substrate are not quantum dots. Consequently, IPL of SiC-dots can be improved in a Si substrate with higher NS. |
doi_str_mv | 10.1063/5.0077886 |
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Transmission electron microscopy observation and x-ray photoelectron spectroscopy revealed the formation of SiC-dots in the (110)- and (111)-C+–Si, in addition to (100)-C+–Si. The diameter (Φ) and surface density (ND) of the SiC-dots depended on the Si surface orientation, and the average Φ of the SiC-dots in three surface-oriented C+–Si decreased from approximately 5–3 nm with increasing NS because the trapping value of C-ions at SiO2/Si interface increased with increasing NS, which leads to the reduction of C-ions to convert SiC-dots in the SiC-dot formation area under higher NS condition. However, the UV-Raman intensity of the TO mode of Si−C vibration was nearly independent of NS. We experimentally confirmed the PL emissions from the (110)- and (111)-C+–Si in addition to the (100)-C+–Si. As a result, the PL spectrum and PL emission coefficient (η) of the SiC-dots strongly depended on the Si surface orientation. The PL intensity IPL of the SiC-dots strongly depended on the NS because the η of the SiC-dots significantly increased with decreasing Φ, although SiC-dots in Si substrate are not quantum dots. Consequently, IPL of SiC-dots can be improved in a Si substrate with higher NS.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/5.0077886</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Bulk density ; Ion implantation ; Orientation ; Photoelectrons ; Photoluminescence ; Quantum dots ; Silicon dioxide ; Silicon substrates</subject><ispartof>Journal of applied physics, 2022-02, Vol.131 (7)</ispartof><rights>Author(s)</rights><rights>2022 Author(s). Published under an exclusive license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c257t-3530a3a47558853e71e291f85d73ec1752dac7e2bf0c4fdded48a062586c00783</citedby><cites>FETCH-LOGICAL-c257t-3530a3a47558853e71e291f85d73ec1752dac7e2bf0c4fdded48a062586c00783</cites><orcidid>0000-0001-8039-4940 ; 0000-0003-2915-2385</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/10.1063/5.0077886$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>315,781,785,795,4513,27929,27930,76389</link.rule.ids></links><search><creatorcontrib>Mizuno, Tomohisa</creatorcontrib><creatorcontrib>Aoki, Takashi</creatorcontrib><creatorcontrib>Sameshima, Toshiyuki</creatorcontrib><title>Si surface orientation dependence of SiC-dot formation in bulk-Si using hot-C+-ion implantation technique</title><title>Journal of applied physics</title><description>We experimentally investigated the Si surface orientation dependence of SiC-dot formation and photoluminescence (PL) properties in three (100)-, (110)-, and (111)-bulk-Si substrates (C+–Si) with different surface densities of Si atoms (NS), where SiC-dots were fabricated by a hot-C+ ion implantation into bulk-Si and post-N2 annealing processes. Transmission electron microscopy observation and x-ray photoelectron spectroscopy revealed the formation of SiC-dots in the (110)- and (111)-C+–Si, in addition to (100)-C+–Si. The diameter (Φ) and surface density (ND) of the SiC-dots depended on the Si surface orientation, and the average Φ of the SiC-dots in three surface-oriented C+–Si decreased from approximately 5–3 nm with increasing NS because the trapping value of C-ions at SiO2/Si interface increased with increasing NS, which leads to the reduction of C-ions to convert SiC-dots in the SiC-dot formation area under higher NS condition. However, the UV-Raman intensity of the TO mode of Si−C vibration was nearly independent of NS. We experimentally confirmed the PL emissions from the (110)- and (111)-C+–Si in addition to the (100)-C+–Si. As a result, the PL spectrum and PL emission coefficient (η) of the SiC-dots strongly depended on the Si surface orientation. The PL intensity IPL of the SiC-dots strongly depended on the NS because the η of the SiC-dots significantly increased with decreasing Φ, although SiC-dots in Si substrate are not quantum dots. Consequently, IPL of SiC-dots can be improved in a Si substrate with higher NS.</description><subject>Applied physics</subject><subject>Bulk density</subject><subject>Ion implantation</subject><subject>Orientation</subject><subject>Photoelectrons</subject><subject>Photoluminescence</subject><subject>Quantum dots</subject><subject>Silicon dioxide</subject><subject>Silicon substrates</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNqdkMtOwzAQRS0EEqWw4A8isQLk4kccO0sU8ZIqsSisLdcP6tLGwU6Q-HtcUsSe1Uhzz9w7MwCcYzTDqKI3bIYQ50JUB2CCkaghZwwdgglCBENR8_oYnKS0RghjQesJ8AtfpCE6pW0Rordtr3of2sLYzrbGtru2Kxa-gSb0hQtxO-q-LZbD5h3m8SH59q1YhR421_BH23Yb9WvUW71q_cdgT8GRU5tkz_Z1Cl7v716aRzh_fnhqbudQE8Z7SBlFiqoy7y0Eo5ZjS2rsBDOcWo05I0ZpbsnSIV06Y6wphUIVYaLS-XRBp-Bi9O1iyLGpl-swxDZHSlJlq5KQus7U5UjpGFKK1sku-q2KXxIjufukZHL_ycxejWzSfrzqf_BniH-g7Iyj3_ZQgaM</recordid><startdate>20220221</startdate><enddate>20220221</enddate><creator>Mizuno, Tomohisa</creator><creator>Aoki, Takashi</creator><creator>Sameshima, Toshiyuki</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-8039-4940</orcidid><orcidid>https://orcid.org/0000-0003-2915-2385</orcidid></search><sort><creationdate>20220221</creationdate><title>Si surface orientation dependence of SiC-dot formation in bulk-Si using hot-C+-ion implantation technique</title><author>Mizuno, Tomohisa ; Aoki, Takashi ; Sameshima, Toshiyuki</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c257t-3530a3a47558853e71e291f85d73ec1752dac7e2bf0c4fdded48a062586c00783</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Applied physics</topic><topic>Bulk density</topic><topic>Ion implantation</topic><topic>Orientation</topic><topic>Photoelectrons</topic><topic>Photoluminescence</topic><topic>Quantum dots</topic><topic>Silicon dioxide</topic><topic>Silicon substrates</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Mizuno, Tomohisa</creatorcontrib><creatorcontrib>Aoki, Takashi</creatorcontrib><creatorcontrib>Sameshima, Toshiyuki</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mizuno, Tomohisa</au><au>Aoki, Takashi</au><au>Sameshima, Toshiyuki</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Si surface orientation dependence of SiC-dot formation in bulk-Si using hot-C+-ion implantation technique</atitle><jtitle>Journal of applied physics</jtitle><date>2022-02-21</date><risdate>2022</risdate><volume>131</volume><issue>7</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>We experimentally investigated the Si surface orientation dependence of SiC-dot formation and photoluminescence (PL) properties in three (100)-, (110)-, and (111)-bulk-Si substrates (C+–Si) with different surface densities of Si atoms (NS), where SiC-dots were fabricated by a hot-C+ ion implantation into bulk-Si and post-N2 annealing processes. Transmission electron microscopy observation and x-ray photoelectron spectroscopy revealed the formation of SiC-dots in the (110)- and (111)-C+–Si, in addition to (100)-C+–Si. The diameter (Φ) and surface density (ND) of the SiC-dots depended on the Si surface orientation, and the average Φ of the SiC-dots in three surface-oriented C+–Si decreased from approximately 5–3 nm with increasing NS because the trapping value of C-ions at SiO2/Si interface increased with increasing NS, which leads to the reduction of C-ions to convert SiC-dots in the SiC-dot formation area under higher NS condition. However, the UV-Raman intensity of the TO mode of Si−C vibration was nearly independent of NS. We experimentally confirmed the PL emissions from the (110)- and (111)-C+–Si in addition to the (100)-C+–Si. As a result, the PL spectrum and PL emission coefficient (η) of the SiC-dots strongly depended on the Si surface orientation. The PL intensity IPL of the SiC-dots strongly depended on the NS because the η of the SiC-dots significantly increased with decreasing Φ, although SiC-dots in Si substrate are not quantum dots. Consequently, IPL of SiC-dots can be improved in a Si substrate with higher NS.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0077886</doi><tpages>13</tpages><orcidid>https://orcid.org/0000-0001-8039-4940</orcidid><orcidid>https://orcid.org/0000-0003-2915-2385</orcidid></addata></record> |
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source | AIP Journals Complete; Alma/SFX Local Collection |
subjects | Applied physics Bulk density Ion implantation Orientation Photoelectrons Photoluminescence Quantum dots Silicon dioxide Silicon substrates |
title | Si surface orientation dependence of SiC-dot formation in bulk-Si using hot-C+-ion implantation technique |
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