Magnesium acceptor in gallium nitride. I. Photoluminescence from Mg-doped GaN
Defect-related photoluminescence (PL) is analyzed in detail for n-type, p-type, and semi-insulating Mg-doped GaN grown by different techniques. The ultraviolet luminescence (UVL) band is the dominant PL band in conductive n-type and p-type GaN:Mg samples grown by hydride vapor phase epitaxy (HVPE) a...
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description | Defect-related photoluminescence (PL) is analyzed in detail for n-type, p-type, and semi-insulating Mg-doped GaN grown by different techniques. The ultraviolet luminescence (UVL) band is the dominant PL band in conductive n-type and p-type GaN:Mg samples grown by hydride vapor phase epitaxy (HVPE) and molecular beam epitaxy. The UVL band in undoped and Mg-doped GaN samples is attributed to the shallow MgGa acceptor with the ionization energy of 223 meV. In semi-insulating GaN:Mg samples, very large shifts of the UVL band (up to 0.6 eV) are observed with variation of temperature or excitation intensity. The shifts are attributed to diagonal transitions, likely due to potential fluctuations or near-surface band bending. The blue luminescence (BLMg) band is observed only in GaN:Mg samples grown by HVPE or metalorganic chemical vapor deposition when the concentration of Mg exceeds 1019cm−3. The BLMg band is attributed to electron transitions from an unknown deep donor to the shallow MgGa acceptor. Basic properties of the observed PL are explained with a phenomenological model. |
doi_str_mv | 10.1103/PhysRevB.97.205204 |
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Photoluminescence from Mg-doped GaN</title><source>American Physical Society Journals</source><creator>Reshchikov, M A ; Ghimire, P ; Demchenko, D O</creator><creatorcontrib>Reshchikov, M A ; Ghimire, P ; Demchenko, D O</creatorcontrib><description>Defect-related photoluminescence (PL) is analyzed in detail for n-type, p-type, and semi-insulating Mg-doped GaN grown by different techniques. The ultraviolet luminescence (UVL) band is the dominant PL band in conductive n-type and p-type GaN:Mg samples grown by hydride vapor phase epitaxy (HVPE) and molecular beam epitaxy. The UVL band in undoped and Mg-doped GaN samples is attributed to the shallow MgGa acceptor with the ionization energy of 223 meV. In semi-insulating GaN:Mg samples, very large shifts of the UVL band (up to 0.6 eV) are observed with variation of temperature or excitation intensity. The shifts are attributed to diagonal transitions, likely due to potential fluctuations or near-surface band bending. The blue luminescence (BLMg) band is observed only in GaN:Mg samples grown by HVPE or metalorganic chemical vapor deposition when the concentration of Mg exceeds 1019cm−3. The BLMg band is attributed to electron transitions from an unknown deep donor to the shallow MgGa acceptor. Basic properties of the observed PL are explained with a phenomenological model.</description><identifier>ISSN: 2469-9950</identifier><identifier>EISSN: 2469-9969</identifier><identifier>DOI: 10.1103/PhysRevB.97.205204</identifier><language>eng</language><publisher>College Park: American Physical Society</publisher><subject>Electron transitions ; Epitaxial growth ; Gallium nitrides ; Ionization ; Luminescence ; Magnesium ; Metalorganic chemical vapor deposition ; Molecular beam epitaxy ; Organic chemistry ; Photoluminescence ; Vapor phase epitaxy ; Vapor phases ; Variations</subject><ispartof>Physical review. 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The ultraviolet luminescence (UVL) band is the dominant PL band in conductive n-type and p-type GaN:Mg samples grown by hydride vapor phase epitaxy (HVPE) and molecular beam epitaxy. The UVL band in undoped and Mg-doped GaN samples is attributed to the shallow MgGa acceptor with the ionization energy of 223 meV. In semi-insulating GaN:Mg samples, very large shifts of the UVL band (up to 0.6 eV) are observed with variation of temperature or excitation intensity. The shifts are attributed to diagonal transitions, likely due to potential fluctuations or near-surface band bending. The blue luminescence (BLMg) band is observed only in GaN:Mg samples grown by HVPE or metalorganic chemical vapor deposition when the concentration of Mg exceeds 1019cm−3. The BLMg band is attributed to electron transitions from an unknown deep donor to the shallow MgGa acceptor. Basic properties of the observed PL are explained with a phenomenological model.</description><subject>Electron transitions</subject><subject>Epitaxial growth</subject><subject>Gallium nitrides</subject><subject>Ionization</subject><subject>Luminescence</subject><subject>Magnesium</subject><subject>Metalorganic chemical vapor deposition</subject><subject>Molecular beam epitaxy</subject><subject>Organic chemistry</subject><subject>Photoluminescence</subject><subject>Vapor phase epitaxy</subject><subject>Vapor phases</subject><subject>Variations</subject><issn>2469-9950</issn><issn>2469-9969</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNo9jtFLwzAYxIMoOOb-AZ8CPrd-SZq0edShc7DqEH0eafK162ib2rSC_70Vxac7jh93R8g1g5gxELf741d4xc_7WKcxB8khOSMLnigdaa30-b-XcElWIZwAgCnQKegFyXNTdRjqqaXGWuxHP9C6o5Vpmp-sq8ehdhjTbUz3Rz_6ZmrrmbfYWaTl4FuaV5HzPTq6Mc9X5KI0TcDVny7J--PD2_op2r1stuu7XdQzJsZIKxASHc5XpXUpOJ05wUthXKKKwjiniqxwSqQGFU8BjLbKInChlNRcFmJJbn57-8F_TBjGw8lPQzdPHjjjgmWQci6-AdODUcY</recordid><startdate>20180517</startdate><enddate>20180517</enddate><creator>Reshchikov, M A</creator><creator>Ghimire, P</creator><creator>Demchenko, D O</creator><general>American Physical Society</general><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>H8D</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20180517</creationdate><title>Magnesium acceptor in gallium nitride. I. Photoluminescence from Mg-doped GaN</title><author>Reshchikov, M A ; Ghimire, P ; Demchenko, D O</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p113t-96035ede5205cd70d98d32f3ad46bbadd6b8bd637ae62700a9c6ce023665925b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Electron transitions</topic><topic>Epitaxial growth</topic><topic>Gallium nitrides</topic><topic>Ionization</topic><topic>Luminescence</topic><topic>Magnesium</topic><topic>Metalorganic chemical vapor deposition</topic><topic>Molecular beam epitaxy</topic><topic>Organic chemistry</topic><topic>Photoluminescence</topic><topic>Vapor phase epitaxy</topic><topic>Vapor phases</topic><topic>Variations</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Reshchikov, M A</creatorcontrib><creatorcontrib>Ghimire, P</creatorcontrib><creatorcontrib>Demchenko, D O</creatorcontrib><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physical review. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Reshchikov, M A</au><au>Ghimire, P</au><au>Demchenko, D O</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Magnesium acceptor in gallium nitride. I. Photoluminescence from Mg-doped GaN</atitle><jtitle>Physical review. B</jtitle><date>2018-05-17</date><risdate>2018</risdate><volume>97</volume><issue>20</issue><issn>2469-9950</issn><eissn>2469-9969</eissn><abstract>Defect-related photoluminescence (PL) is analyzed in detail for n-type, p-type, and semi-insulating Mg-doped GaN grown by different techniques. The ultraviolet luminescence (UVL) band is the dominant PL band in conductive n-type and p-type GaN:Mg samples grown by hydride vapor phase epitaxy (HVPE) and molecular beam epitaxy. The UVL band in undoped and Mg-doped GaN samples is attributed to the shallow MgGa acceptor with the ionization energy of 223 meV. In semi-insulating GaN:Mg samples, very large shifts of the UVL band (up to 0.6 eV) are observed with variation of temperature or excitation intensity. The shifts are attributed to diagonal transitions, likely due to potential fluctuations or near-surface band bending. The blue luminescence (BLMg) band is observed only in GaN:Mg samples grown by HVPE or metalorganic chemical vapor deposition when the concentration of Mg exceeds 1019cm−3. The BLMg band is attributed to electron transitions from an unknown deep donor to the shallow MgGa acceptor. Basic properties of the observed PL are explained with a phenomenological model.</abstract><cop>College Park</cop><pub>American Physical Society</pub><doi>10.1103/PhysRevB.97.205204</doi><oa>free_for_read</oa></addata></record> |
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subjects | Electron transitions Epitaxial growth Gallium nitrides Ionization Luminescence Magnesium Metalorganic chemical vapor deposition Molecular beam epitaxy Organic chemistry Photoluminescence Vapor phase epitaxy Vapor phases Variations |
title | Magnesium acceptor in gallium nitride. I. Photoluminescence from Mg-doped GaN |
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