Crystal Phase-Selective Epitaxy of Rutile and Anatase Nb-Doped TiO2 Films on a GaN Template by the Helicon-Wave-Excited-Plasma Sputtering Epitaxy Method
Crystal phase-selective epitaxy of Nb-doped TiO 2 (TiO 2 :Nb) films on GaN is demonstrated using the helicon-wave-excited-plasma sputtering epitaxy method. On the clean (0001) GaN, rutile (100) TiO 2 :Nb was grown regardless of growth temperature ($T_{\text{g}}$). On the (0001) GaN covered with a mo...
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Veröffentlicht in: | Applied physics express 2010-09, Vol.3 (9), p.091102-091102-3 |
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description | Crystal phase-selective epitaxy of Nb-doped TiO 2 (TiO 2 :Nb) films on GaN is demonstrated using the helicon-wave-excited-plasma sputtering epitaxy method. On the clean (0001) GaN, rutile (100) TiO 2 :Nb was grown regardless of growth temperature ($T_{\text{g}}$). On the (0001) GaN covered with a monolayer-thick (100) or (001) $\beta$-Ga 2 O 3 , anatase (001) TiO 2 :Nb was grown with the in-plane relation $\langle 110\rangle$TiO 2 $\parallel$ $\langle 11\bar{2}0\rangle$GaN under high $T_{\text{g}}$ and low O 2 partial pressure conditions. The transmittance between 450 and 900 nm for the 200-nm-thick films was approximately 80%. Typical resistivity of the anatase TiO 2 :Nb/GaN heterostructure was as low as $3.6\times 10^{-4}$ $\Omega$$\cdot$cm, due to the interfacial conduction. |
doi_str_mv | 10.1143/APEX.3.091102 |
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On the clean (0001) GaN, rutile (100) TiO 2 :Nb was grown regardless of growth temperature ($T_{\text{g}}$). On the (0001) GaN covered with a monolayer-thick (100) or (001) $\beta$-Ga 2 O 3 , anatase (001) TiO 2 :Nb was grown with the in-plane relation $\langle 110\rangle$TiO 2 $\parallel$ $\langle 11\bar{2}0\rangle$GaN under high $T_{\text{g}}$ and low O 2 partial pressure conditions. The transmittance between 450 and 900 nm for the 200-nm-thick films was approximately 80%. Typical resistivity of the anatase TiO 2 :Nb/GaN heterostructure was as low as $3.6\times 10^{-4}$ $\Omega$$\cdot$cm, due to the interfacial conduction.</description><identifier>ISSN: 1882-0778</identifier><identifier>EISSN: 1882-0786</identifier><identifier>DOI: 10.1143/APEX.3.091102</identifier><language>eng</language><publisher>The Japan Society of Applied Physics</publisher><ispartof>Applied physics express, 2010-09, Vol.3 (9), p.091102-091102-3</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Hazu, Kouji</creatorcontrib><creatorcontrib>Fouda, Aly</creatorcontrib><creatorcontrib>Nakayama, Tokuyuki</creatorcontrib><creatorcontrib>Tanaka, Akikazu</creatorcontrib><creatorcontrib>Chichibu, Shigefusa F</creatorcontrib><title>Crystal Phase-Selective Epitaxy of Rutile and Anatase Nb-Doped TiO2 Films on a GaN Template by the Helicon-Wave-Excited-Plasma Sputtering Epitaxy Method</title><title>Applied physics express</title><description>Crystal phase-selective epitaxy of Nb-doped TiO 2 (TiO 2 :Nb) films on GaN is demonstrated using the helicon-wave-excited-plasma sputtering epitaxy method. On the clean (0001) GaN, rutile (100) TiO 2 :Nb was grown regardless of growth temperature ($T_{\text{g}}$). On the (0001) GaN covered with a monolayer-thick (100) or (001) $\beta$-Ga 2 O 3 , anatase (001) TiO 2 :Nb was grown with the in-plane relation $\langle 110\rangle$TiO 2 $\parallel$ $\langle 11\bar{2}0\rangle$GaN under high $T_{\text{g}}$ and low O 2 partial pressure conditions. The transmittance between 450 and 900 nm for the 200-nm-thick films was approximately 80%. Typical resistivity of the anatase TiO 2 :Nb/GaN heterostructure was as low as $3.6\times 10^{-4}$ $\Omega$$\cdot$cm, due to the interfacial conduction.</description><issn>1882-0778</issn><issn>1882-0786</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNo9kM1OwkAYRSdGExFduv-2Lgbnj3a6JFjABIEIRnfNtPNVxvQvdCD0TXxcJRpW9y5uzk0OIfecDThX8nG0ij8GcsAizpm4ID2utaAs1MHluYf6mty07RdjgZI86JHv8a5rvSlgtTUt0jUWmHl3QIgb582xgzqH1713BYKpLIwq4393sEjpU92ghY1bCpi4omyhrsDA1Cxgg2VTGI-QduC3CDMsXFZX9N0ckMbHzHm0dFWYtjSwbvbe485Vn-fHF_Tb2t6Sq9wULd79Z5-8TeLNeEbny-nzeDSnTnDuqcpZpEIZBDZUwwwtF8paFaGyQcrTjIcmFMLmkRAYWJ5GURpJLTXTw0xYHWSyTx7-uK4xTdLsXGl2XcJZclKanJQmMvlTKn8A5Dpp3Q</recordid><startdate>201009</startdate><enddate>201009</enddate><creator>Hazu, Kouji</creator><creator>Fouda, Aly</creator><creator>Nakayama, Tokuyuki</creator><creator>Tanaka, Akikazu</creator><creator>Chichibu, Shigefusa F</creator><general>The Japan Society of Applied Physics</general><scope/></search><sort><creationdate>201009</creationdate><title>Crystal Phase-Selective Epitaxy of Rutile and Anatase Nb-Doped TiO2 Films on a GaN Template by the Helicon-Wave-Excited-Plasma Sputtering Epitaxy Method</title><author>Hazu, Kouji ; Fouda, Aly ; Nakayama, Tokuyuki ; Tanaka, Akikazu ; Chichibu, Shigefusa F</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i211t-4f0947366d745ced124dd49e4d6b1bc17a722df922e6d1b99b93838085c2d86c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Hazu, Kouji</creatorcontrib><creatorcontrib>Fouda, Aly</creatorcontrib><creatorcontrib>Nakayama, Tokuyuki</creatorcontrib><creatorcontrib>Tanaka, Akikazu</creatorcontrib><creatorcontrib>Chichibu, Shigefusa F</creatorcontrib><jtitle>Applied physics express</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Hazu, Kouji</au><au>Fouda, Aly</au><au>Nakayama, Tokuyuki</au><au>Tanaka, Akikazu</au><au>Chichibu, Shigefusa F</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Crystal Phase-Selective Epitaxy of Rutile and Anatase Nb-Doped TiO2 Films on a GaN Template by the Helicon-Wave-Excited-Plasma Sputtering Epitaxy Method</atitle><jtitle>Applied physics express</jtitle><date>2010-09</date><risdate>2010</risdate><volume>3</volume><issue>9</issue><spage>091102</spage><epage>091102-3</epage><pages>091102-091102-3</pages><issn>1882-0778</issn><eissn>1882-0786</eissn><abstract>Crystal phase-selective epitaxy of Nb-doped TiO 2 (TiO 2 :Nb) films on GaN is demonstrated using the helicon-wave-excited-plasma sputtering epitaxy method. On the clean (0001) GaN, rutile (100) TiO 2 :Nb was grown regardless of growth temperature ($T_{\text{g}}$). On the (0001) GaN covered with a monolayer-thick (100) or (001) $\beta$-Ga 2 O 3 , anatase (001) TiO 2 :Nb was grown with the in-plane relation $\langle 110\rangle$TiO 2 $\parallel$ $\langle 11\bar{2}0\rangle$GaN under high $T_{\text{g}}$ and low O 2 partial pressure conditions. The transmittance between 450 and 900 nm for the 200-nm-thick films was approximately 80%. Typical resistivity of the anatase TiO 2 :Nb/GaN heterostructure was as low as $3.6\times 10^{-4}$ $\Omega$$\cdot$cm, due to the interfacial conduction.</abstract><pub>The Japan Society of Applied Physics</pub><doi>10.1143/APEX.3.091102</doi></addata></record> |
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title | Crystal Phase-Selective Epitaxy of Rutile and Anatase Nb-Doped TiO2 Films on a GaN Template by the Helicon-Wave-Excited-Plasma Sputtering Epitaxy Method |
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