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Valency configuration of transition metal impurities in ZnO
We use the self-interaction corrected local spin-density approximation to investigate the ground state valency configuration of transition metal (TM = Mn, Co) impurities in n- and p-type ZnO. We find that in pure Zn^sub 1-x^TM^sub x^O, the localized TM^sup 2+^ configuration is energetically favored...
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Published in: | Journal of electronic materials 2006-04, Vol.35 (4), p.556-561 |
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container_title | Journal of electronic materials |
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creator | Petit, L Schulthess, T C Svane, A Temmerman, W M Szotek, Z Janotti, A |
description | We use the self-interaction corrected local spin-density approximation to investigate the ground state valency configuration of transition metal (TM = Mn, Co) impurities in n- and p-type ZnO. We find that in pure Zn^sub 1-x^TM^sub x^O, the localized TM^sup 2+^ configuration is energetically favored over the itinerant d-electron configuration of the local spin density (LSD) picture. Our calculations indicate furthermore that the (+/0) donor level is situated in the ZnO gap. Consequently, for n-type conditions, with the Fermi energy ε^sub F^ close to the conduction band minimum, TM remains in the 2+ charge state, while for p-type conditions, with ε^sub F^ close to the valence band maximum, the 3+ charge state is energetically preferred. In the latter scenario, modeled here by co-doping with N, the additional delocalized d-electron charge transfers into the entire states at the top of the valence band, and hole carriers will only exist, if the N concentration exceeds the TM impurity concentration. [PUBLICATION ABSTRACT] |
doi_str_mv | 10.1007/s11664-006-0099-8 |
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(ORNL), Oak Ridge, TN (United States) ; Center for Computational Sciences</creatorcontrib><description>We use the self-interaction corrected local spin-density approximation to investigate the ground state valency configuration of transition metal (TM = Mn, Co) impurities in n- and p-type ZnO. We find that in pure Zn^sub 1-x^TM^sub x^O, the localized TM^sup 2+^ configuration is energetically favored over the itinerant d-electron configuration of the local spin density (LSD) picture. Our calculations indicate furthermore that the (+/0) donor level is situated in the ZnO gap. Consequently, for n-type conditions, with the Fermi energy ε^sub F^ close to the conduction band minimum, TM remains in the 2+ charge state, while for p-type conditions, with ε^sub F^ close to the valence band maximum, the 3+ charge state is energetically preferred. In the latter scenario, modeled here by co-doping with N, the additional delocalized d-electron charge transfers into the entire states at the top of the valence band, and hole carriers will only exist, if the N concentration exceeds the TM impurity concentration. [PUBLICATION ABSTRACT]</description><identifier>ISSN: 0361-5235</identifier><identifier>EISSN: 1543-186X</identifier><identifier>DOI: 10.1007/s11664-006-0099-8</identifier><identifier>CODEN: JECMA5</identifier><language>eng</language><publisher>Warrendale: Springer Nature B.V</publisher><subject>APPROXIMATIONS ; CHARGE STATES ; Charge transfer ; Conduction bands ; CONFIGURATION ; Configurations ; Density ; Electromagnetism ; Electron spin ; Electrons ; GROUND STATES ; IMPURITIES ; MATERIALS SCIENCE ; Semiconductors ; SPIN ; TRANSITION ELEMENTS ; Transition metals ; VALENCE ; Valence band ; Zinc oxide ; Zinc oxides</subject><ispartof>Journal of electronic materials, 2006-04, Vol.35 (4), p.556-561</ispartof><rights>Copyright Minerals, Metals & Materials Society Apr 2006</rights><rights>TMS-The Minerals, Metals and Materials Society 2006.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c358t-a339a12d4f3e3d85e635bc66e3d6de9454715fc507d686bceecfa14314c218453</citedby><cites>FETCH-LOGICAL-c358t-a339a12d4f3e3d85e635bc66e3d6de9454715fc507d686bceecfa14314c218453</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/1003292$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Petit, L</creatorcontrib><creatorcontrib>Schulthess, T C</creatorcontrib><creatorcontrib>Svane, A</creatorcontrib><creatorcontrib>Temmerman, W M</creatorcontrib><creatorcontrib>Szotek, Z</creatorcontrib><creatorcontrib>Janotti, A</creatorcontrib><creatorcontrib>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</creatorcontrib><creatorcontrib>Center for Computational Sciences</creatorcontrib><title>Valency configuration of transition metal impurities in ZnO</title><title>Journal of electronic materials</title><description>We use the self-interaction corrected local spin-density approximation to investigate the ground state valency configuration of transition metal (TM = Mn, Co) impurities in n- and p-type ZnO. We find that in pure Zn^sub 1-x^TM^sub x^O, the localized TM^sup 2+^ configuration is energetically favored over the itinerant d-electron configuration of the local spin density (LSD) picture. Our calculations indicate furthermore that the (+/0) donor level is situated in the ZnO gap. Consequently, for n-type conditions, with the Fermi energy ε^sub F^ close to the conduction band minimum, TM remains in the 2+ charge state, while for p-type conditions, with ε^sub F^ close to the valence band maximum, the 3+ charge state is energetically preferred. In the latter scenario, modeled here by co-doping with N, the additional delocalized d-electron charge transfers into the entire states at the top of the valence band, and hole carriers will only exist, if the N concentration exceeds the TM impurity concentration. [PUBLICATION ABSTRACT]</description><subject>APPROXIMATIONS</subject><subject>CHARGE STATES</subject><subject>Charge transfer</subject><subject>Conduction bands</subject><subject>CONFIGURATION</subject><subject>Configurations</subject><subject>Density</subject><subject>Electromagnetism</subject><subject>Electron spin</subject><subject>Electrons</subject><subject>GROUND STATES</subject><subject>IMPURITIES</subject><subject>MATERIALS SCIENCE</subject><subject>Semiconductors</subject><subject>SPIN</subject><subject>TRANSITION ELEMENTS</subject><subject>Transition metals</subject><subject>VALENCE</subject><subject>Valence band</subject><subject>Zinc oxide</subject><subject>Zinc oxides</subject><issn>0361-5235</issn><issn>1543-186X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><recordid>eNptkU1LAzEQhoMoWKs_wNui4G01k69N8CTFLyj0oiJeQprNaso2W5PdQ_-9qSsI4mEYZniYed8ZhE4BXwLG1VUCEIKVGIscSpVyD02AM1qCFK_7aIKpgJITyg_RUUorjIGDhAm6fjGtC3Zb2C40_n2IpvddKLqm6KMJyX9Xa9ebtvDrzRBzw6XCh-ItLI7RQWPa5E5-8hQ9390-zR7K-eL-cXYzLy3lsi8NpcoAqVlDHa0ld4LypRUiF6J2inFWAW8sx1UtpFha52xjgFFgloBknE7R2Ti3S73Xyfre2Y-sNzjb6-yeEkUydDFCm9h9Di71eu2TdW1rguuGpIlSEojEGTz_A666IYZsQJN8wiqfkJLfnf9QmCmCFdlBMEI2dilF1-hN9GsTt1nVTlilx7foPFPv3qIl_QKw733A</recordid><startdate>20060401</startdate><enddate>20060401</enddate><creator>Petit, L</creator><creator>Schulthess, T C</creator><creator>Svane, A</creator><creator>Temmerman, W M</creator><creator>Szotek, Z</creator><creator>Janotti, A</creator><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7XB</scope><scope>88I</scope><scope>8AF</scope><scope>8AO</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>8G5</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>GNUQQ</scope><scope>GUQSH</scope><scope>HCIFZ</scope><scope>KB.</scope><scope>L6V</scope><scope>M2O</scope><scope>M2P</scope><scope>M7S</scope><scope>MBDVC</scope><scope>P5Z</scope><scope>P62</scope><scope>PDBOC</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>Q9U</scope><scope>S0X</scope><scope>7QQ</scope><scope>7SP</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20060401</creationdate><title>Valency configuration of transition metal impurities in ZnO</title><author>Petit, L ; Schulthess, T C ; Svane, A ; Temmerman, W M ; Szotek, Z ; Janotti, A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c358t-a339a12d4f3e3d85e635bc66e3d6de9454715fc507d686bceecfa14314c218453</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2006</creationdate><topic>APPROXIMATIONS</topic><topic>CHARGE STATES</topic><topic>Charge transfer</topic><topic>Conduction bands</topic><topic>CONFIGURATION</topic><topic>Configurations</topic><topic>Density</topic><topic>Electromagnetism</topic><topic>Electron spin</topic><topic>Electrons</topic><topic>GROUND STATES</topic><topic>IMPURITIES</topic><topic>MATERIALS SCIENCE</topic><topic>Semiconductors</topic><topic>SPIN</topic><topic>TRANSITION ELEMENTS</topic><topic>Transition metals</topic><topic>VALENCE</topic><topic>Valence band</topic><topic>Zinc oxide</topic><topic>Zinc oxides</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Petit, L</creatorcontrib><creatorcontrib>Schulthess, T C</creatorcontrib><creatorcontrib>Svane, A</creatorcontrib><creatorcontrib>Temmerman, W M</creatorcontrib><creatorcontrib>Szotek, Z</creatorcontrib><creatorcontrib>Janotti, A</creatorcontrib><creatorcontrib>Oak Ridge National Lab. 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(ORNL), Oak Ridge, TN (United States)</aucorp><aucorp>Center for Computational Sciences</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Valency configuration of transition metal impurities in ZnO</atitle><jtitle>Journal of electronic materials</jtitle><date>2006-04-01</date><risdate>2006</risdate><volume>35</volume><issue>4</issue><spage>556</spage><epage>561</epage><pages>556-561</pages><issn>0361-5235</issn><eissn>1543-186X</eissn><coden>JECMA5</coden><abstract>We use the self-interaction corrected local spin-density approximation to investigate the ground state valency configuration of transition metal (TM = Mn, Co) impurities in n- and p-type ZnO. We find that in pure Zn^sub 1-x^TM^sub x^O, the localized TM^sup 2+^ configuration is energetically favored over the itinerant d-electron configuration of the local spin density (LSD) picture. Our calculations indicate furthermore that the (+/0) donor level is situated in the ZnO gap. Consequently, for n-type conditions, with the Fermi energy ε^sub F^ close to the conduction band minimum, TM remains in the 2+ charge state, while for p-type conditions, with ε^sub F^ close to the valence band maximum, the 3+ charge state is energetically preferred. In the latter scenario, modeled here by co-doping with N, the additional delocalized d-electron charge transfers into the entire states at the top of the valence band, and hole carriers will only exist, if the N concentration exceeds the TM impurity concentration. [PUBLICATION ABSTRACT]</abstract><cop>Warrendale</cop><pub>Springer Nature B.V</pub><doi>10.1007/s11664-006-0099-8</doi><tpages>6</tpages></addata></record> |
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subjects | APPROXIMATIONS CHARGE STATES Charge transfer Conduction bands CONFIGURATION Configurations Density Electromagnetism Electron spin Electrons GROUND STATES IMPURITIES MATERIALS SCIENCE Semiconductors SPIN TRANSITION ELEMENTS Transition metals VALENCE Valence band Zinc oxide Zinc oxides |
title | Valency configuration of transition metal impurities in ZnO |
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