Iron and manganese doped zinc-blende GaN
The electronic structure of Mn and Fe doping impurities in zinc-blende gallium nitride (c-GaN) crystal lattice have been investigated by the LMTO-TB method. The calculations used the 128 site supercells (64 atoms and 64 empty spheres with an impurity at the origin) with Mn and Fe atoms replacing ion...
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Veröffentlicht in: | Journal of electronic materials 2000-09, Vol.29 (9), p.1067-1073 |
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description | The electronic structure of Mn and Fe doping impurities in zinc-blende gallium nitride (c-GaN) crystal lattice have been investigated by the LMTO-TB method. The calculations used the 128 site supercells (64 atoms and 64 empty spheres with an impurity at the origin) with Mn and Fe atoms replacing ions in cation and anion sublattices. It is shown that Mn and Fe ions stay magnetic for all types of substitutions in c-GaN crystal lattice. Fe magnetic moment was found to be 3.5 mu sub(B) and 1.0 mu sub(B) for cation and anion substitutions, respectively. Similar data for Mn, magnetic moments are 3.3 mu sub(B) and 1.9 mu sub(B). The moments are highly localized, though some weak polarization is seen at the closest atoms to the impurity. The total energies for supercells with and without magnetic impurities are used to determine the most probable single substitutional sites for Fe and Mn in c-GaN. The energies of magnetic electrons levels relative to the valence and conduction bands of the host crystal are analyzed by making use of the total and partial densities of states. The results show that combination of optoelectronic and magnetic properties may well be possible for c-GaN iron and Mn doped systems. |
doi_str_mv | 10.1007/s11664-004-0266-8 |
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Y ; GUBANOV, V. A ; BOEKEMA, C</creator><creatorcontrib>FONG, C. Y ; GUBANOV, V. A ; BOEKEMA, C</creatorcontrib><description>The electronic structure of Mn and Fe doping impurities in zinc-blende gallium nitride (c-GaN) crystal lattice have been investigated by the LMTO-TB method. The calculations used the 128 site supercells (64 atoms and 64 empty spheres with an impurity at the origin) with Mn and Fe atoms replacing ions in cation and anion sublattices. It is shown that Mn and Fe ions stay magnetic for all types of substitutions in c-GaN crystal lattice. Fe magnetic moment was found to be 3.5 mu sub(B) and 1.0 mu sub(B) for cation and anion substitutions, respectively. Similar data for Mn, magnetic moments are 3.3 mu sub(B) and 1.9 mu sub(B). The moments are highly localized, though some weak polarization is seen at the closest atoms to the impurity. The total energies for supercells with and without magnetic impurities are used to determine the most probable single substitutional sites for Fe and Mn in c-GaN. The energies of magnetic electrons levels relative to the valence and conduction bands of the host crystal are analyzed by making use of the total and partial densities of states. The results show that combination of optoelectronic and magnetic properties may well be possible for c-GaN iron and Mn doped systems.</description><identifier>ISSN: 0361-5235</identifier><identifier>EISSN: 1543-186X</identifier><identifier>DOI: 10.1007/s11664-004-0266-8</identifier><identifier>CODEN: JECMA5</identifier><language>eng</language><publisher>New York, NY: Institute of Electrical and Electronics Engineers</publisher><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Condensed matter: structure, mechanical and thermal properties ; Defects and impurities in crystals; microstructure ; Diamagnetism, paramagnetism and superparamagnetism ; Doping and impurity implantation in iii-v and ii-vi semiconductors ; Electron states ; Exact sciences and technology ; Iii-v semiconductors ; Impurity and defect levels ; Local moment in compounds and alloys; kondo effect, valence fluctuations, heavy fermions ; Magnetic properties and materials ; Physics ; Structure of solids and liquids; crystallography</subject><ispartof>Journal of electronic materials, 2000-09, Vol.29 (9), p.1067-1073</ispartof><rights>2000 INIST-CNRS</rights><rights>Copyright Minerals, Metals & Materials Society Sep 2000</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c361t-4031cf07b2c9b3c1300dc648f0265a3734e0b9ed648ec6775efc9e4ba07f468b3</citedby><cites>FETCH-LOGICAL-c361t-4031cf07b2c9b3c1300dc648f0265a3734e0b9ed648ec6775efc9e4ba07f468b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=1489877$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>FONG, C. Y</creatorcontrib><creatorcontrib>GUBANOV, V. A</creatorcontrib><creatorcontrib>BOEKEMA, C</creatorcontrib><title>Iron and manganese doped zinc-blende GaN</title><title>Journal of electronic materials</title><description>The electronic structure of Mn and Fe doping impurities in zinc-blende gallium nitride (c-GaN) crystal lattice have been investigated by the LMTO-TB method. The calculations used the 128 site supercells (64 atoms and 64 empty spheres with an impurity at the origin) with Mn and Fe atoms replacing ions in cation and anion sublattices. It is shown that Mn and Fe ions stay magnetic for all types of substitutions in c-GaN crystal lattice. Fe magnetic moment was found to be 3.5 mu sub(B) and 1.0 mu sub(B) for cation and anion substitutions, respectively. Similar data for Mn, magnetic moments are 3.3 mu sub(B) and 1.9 mu sub(B). The moments are highly localized, though some weak polarization is seen at the closest atoms to the impurity. The total energies for supercells with and without magnetic impurities are used to determine the most probable single substitutional sites for Fe and Mn in c-GaN. The energies of magnetic electrons levels relative to the valence and conduction bands of the host crystal are analyzed by making use of the total and partial densities of states. The results show that combination of optoelectronic and magnetic properties may well be possible for c-GaN iron and Mn doped systems.</description><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Defects and impurities in crystals; microstructure</subject><subject>Diamagnetism, paramagnetism and superparamagnetism</subject><subject>Doping and impurity implantation in iii-v and ii-vi semiconductors</subject><subject>Electron states</subject><subject>Exact sciences and technology</subject><subject>Iii-v semiconductors</subject><subject>Impurity and defect levels</subject><subject>Local moment in compounds and alloys; kondo effect, valence fluctuations, heavy fermions</subject><subject>Magnetic properties and materials</subject><subject>Physics</subject><subject>Structure of solids and liquids; crystallography</subject><issn>0361-5235</issn><issn>1543-186X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2000</creationdate><recordtype>article</recordtype><sourceid>8G5</sourceid><sourceid>BENPR</sourceid><sourceid>GUQSH</sourceid><sourceid>M2O</sourceid><recordid>eNqFkEFLAzEQhYMoWKs_wNsiIl6iM5tskj1KqbVQ9KLgLWSziWzZZmvSHvTXm9KC4MXDMDB8b-bNI-QS4Q4B5H1CFIJTgFylEFQdkRFWnFFU4v2YjIAJpFXJqlNyltISACtUOCK38ziEwoS2WJnwYYJLrmiHtWuL7y5Y2vQutK6YmedzcuJNn9zFoY_J2-P0dfJEFy-z-eRhQW2-sKEcGFoPsilt3TCLDKC1giufXVWGScYdNLVr88hZIWXlvK0dbwxIz4Vq2Jjc7Peu4_C5dWmjV12yru-zt2GbdCklKAn4P8iQCS6qDF79AZfDNob8hC6BK4lMQYZwD9k4pBSd1-vYrUz80gh6l7DeJ6xzwnqXsFZZc31YbJI1vY8m2C79CrmqlZTsB68gd_I</recordid><startdate>20000901</startdate><enddate>20000901</enddate><creator>FONG, C. 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A</creatorcontrib><creatorcontrib>BOEKEMA, C</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Science Database (Alumni Edition)</collection><collection>STEM Database</collection><collection>ProQuest Pharma Collection</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>Research Library (Alumni Edition)</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection (ProQuest)</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central Korea</collection><collection>ProQuest Central Student</collection><collection>Research Library Prep</collection><collection>SciTech Premium Collection</collection><collection>Materials Science Database</collection><collection>ProQuest Engineering Collection</collection><collection>Research Library</collection><collection>Science Database</collection><collection>Engineering Database</collection><collection>Research Library (Corporate)</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Materials Science Collection</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>Engineering Collection</collection><collection>ProQuest Central Basic</collection><collection>SIRS Editorial</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Ceramic Abstracts</collection><collection>Materials Research Database</collection><jtitle>Journal of electronic materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>FONG, C. Y</au><au>GUBANOV, V. A</au><au>BOEKEMA, C</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Iron and manganese doped zinc-blende GaN</atitle><jtitle>Journal of electronic materials</jtitle><date>2000-09-01</date><risdate>2000</risdate><volume>29</volume><issue>9</issue><spage>1067</spage><epage>1073</epage><pages>1067-1073</pages><issn>0361-5235</issn><eissn>1543-186X</eissn><coden>JECMA5</coden><abstract>The electronic structure of Mn and Fe doping impurities in zinc-blende gallium nitride (c-GaN) crystal lattice have been investigated by the LMTO-TB method. The calculations used the 128 site supercells (64 atoms and 64 empty spheres with an impurity at the origin) with Mn and Fe atoms replacing ions in cation and anion sublattices. It is shown that Mn and Fe ions stay magnetic for all types of substitutions in c-GaN crystal lattice. Fe magnetic moment was found to be 3.5 mu sub(B) and 1.0 mu sub(B) for cation and anion substitutions, respectively. Similar data for Mn, magnetic moments are 3.3 mu sub(B) and 1.9 mu sub(B). The moments are highly localized, though some weak polarization is seen at the closest atoms to the impurity. The total energies for supercells with and without magnetic impurities are used to determine the most probable single substitutional sites for Fe and Mn in c-GaN. The energies of magnetic electrons levels relative to the valence and conduction bands of the host crystal are analyzed by making use of the total and partial densities of states. The results show that combination of optoelectronic and magnetic properties may well be possible for c-GaN iron and Mn doped systems.</abstract><cop>New York, NY</cop><pub>Institute of Electrical and Electronics Engineers</pub><doi>10.1007/s11664-004-0266-8</doi><tpages>7</tpages></addata></record> |
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subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Condensed matter: structure, mechanical and thermal properties Defects and impurities in crystals microstructure Diamagnetism, paramagnetism and superparamagnetism Doping and impurity implantation in iii-v and ii-vi semiconductors Electron states Exact sciences and technology Iii-v semiconductors Impurity and defect levels Local moment in compounds and alloys kondo effect, valence fluctuations, heavy fermions Magnetic properties and materials Physics Structure of solids and liquids crystallography |
title | Iron and manganese doped zinc-blende GaN |
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