Electron mobility enhancement in n-GaN under Ohmic-metal
We investigated the electron transport properties of n-GaN under an Ohmic-metal. Hall measurement results were compared for n-GaN (A) before Ti-based metal deposition, (B) after Ti-based metal deposition but before annealing, (C) after Ohmic annealing, and (D) after Ohmic-metal removal, where multi-...
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Veröffentlicht in: | AIP advances 2023-07, Vol.13 (7), p.075002-075002-7 |
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creator | Uryu, Kazuya Deng, Yuchen Le, Son Phuong Suzuki, Toshi-kazu |
description | We investigated the electron transport properties of n-GaN under an Ohmic-metal. Hall measurement results were compared for n-GaN (A) before Ti-based metal deposition, (B) after Ti-based metal deposition but before annealing, (C) after Ohmic annealing, and (D) after Ohmic-metal removal, where multi-probe-Hall device measurements are required for (C), while the others, (A), (B), and (D), can be characterized by conventional Hall device measurements. The multi-probe-Hall device measurements for (C) elucidated that, under the Ohmic-metal, the electron concentration is increased and the electron mobility is enhanced in comparison with those for the other cases, (A), (B), and (D). The increased electron concentration indicates that high-density doping takes place in the n-GaN by the Ohmic annealing. However, the high-density doping is not observed after the Ohmic-metal removal. Moreover, the electron mobility enhancement under the Ohmic-metal cannot be explained by donor doping with ionized impurity scattering. These suggest that, under the Ohmic-metal, high-density donors are not formed, and high-density polarization doping owing to strain from the Ohmic-metal takes place. From theoretical calculations, we clarified that the increase in the electron density by polarization doping without donors leads to the suppression of ionized impurity scattering and consequently the electron mobility enhancement. |
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Hall measurement results were compared for n-GaN (A) before Ti-based metal deposition, (B) after Ti-based metal deposition but before annealing, (C) after Ohmic annealing, and (D) after Ohmic-metal removal, where multi-probe-Hall device measurements are required for (C), while the others, (A), (B), and (D), can be characterized by conventional Hall device measurements. The multi-probe-Hall device measurements for (C) elucidated that, under the Ohmic-metal, the electron concentration is increased and the electron mobility is enhanced in comparison with those for the other cases, (A), (B), and (D). The increased electron concentration indicates that high-density doping takes place in the n-GaN by the Ohmic annealing. However, the high-density doping is not observed after the Ohmic-metal removal. Moreover, the electron mobility enhancement under the Ohmic-metal cannot be explained by donor doping with ionized impurity scattering. These suggest that, under the Ohmic-metal, high-density donors are not formed, and high-density polarization doping owing to strain from the Ohmic-metal takes place. From theoretical calculations, we clarified that the increase in the electron density by polarization doping without donors leads to the suppression of ionized impurity scattering and consequently the electron mobility enhancement.</description><identifier>ISSN: 2158-3226</identifier><identifier>EISSN: 2158-3226</identifier><identifier>DOI: 10.1063/5.0147137</identifier><identifier>CODEN: AAIDBI</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Annealing ; Deposition ; Doping ; Electron density ; Electron mobility ; Electron transport ; Gallium nitrides ; Hall effect ; High density ; Impurities ; Polarization ; Scattering ; Titanium ; Transport properties</subject><ispartof>AIP advances, 2023-07, Vol.13 (7), p.075002-075002-7</ispartof><rights>Author(s)</rights><rights>2023 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c391t-9a1fb2c3219ba05d9ef5445a52508b526312b775f7441b91f6397cf6a4d92b663</cites><orcidid>0009-0000-5597-7853 ; 0000-0001-9792-563X ; 0000-0003-4612-8299 ; 0009-0009-6379-7313</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,864,885,2102,27924,27925</link.rule.ids><backlink>$$Uhttps://urn.kb.se/resolve?urn=urn:nbn:se:liu:diva-197589$$DView record from Swedish Publication Index$$Hfree_for_read</backlink></links><search><creatorcontrib>Uryu, Kazuya</creatorcontrib><creatorcontrib>Deng, Yuchen</creatorcontrib><creatorcontrib>Le, Son Phuong</creatorcontrib><creatorcontrib>Suzuki, Toshi-kazu</creatorcontrib><title>Electron mobility enhancement in n-GaN under Ohmic-metal</title><title>AIP advances</title><description>We investigated the electron transport properties of n-GaN under an Ohmic-metal. Hall measurement results were compared for n-GaN (A) before Ti-based metal deposition, (B) after Ti-based metal deposition but before annealing, (C) after Ohmic annealing, and (D) after Ohmic-metal removal, where multi-probe-Hall device measurements are required for (C), while the others, (A), (B), and (D), can be characterized by conventional Hall device measurements. The multi-probe-Hall device measurements for (C) elucidated that, under the Ohmic-metal, the electron concentration is increased and the electron mobility is enhanced in comparison with those for the other cases, (A), (B), and (D). The increased electron concentration indicates that high-density doping takes place in the n-GaN by the Ohmic annealing. However, the high-density doping is not observed after the Ohmic-metal removal. Moreover, the electron mobility enhancement under the Ohmic-metal cannot be explained by donor doping with ionized impurity scattering. These suggest that, under the Ohmic-metal, high-density donors are not formed, and high-density polarization doping owing to strain from the Ohmic-metal takes place. From theoretical calculations, we clarified that the increase in the electron density by polarization doping without donors leads to the suppression of ionized impurity scattering and consequently the electron mobility enhancement.</description><subject>Annealing</subject><subject>Deposition</subject><subject>Doping</subject><subject>Electron density</subject><subject>Electron mobility</subject><subject>Electron transport</subject><subject>Gallium nitrides</subject><subject>Hall effect</subject><subject>High density</subject><subject>Impurities</subject><subject>Polarization</subject><subject>Scattering</subject><subject>Titanium</subject><subject>Transport properties</subject><issn>2158-3226</issn><issn>2158-3226</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>DOA</sourceid><recordid>eNp9kUtLxDAQgIsouKx78B8UPCl0zeTZHGV9grgX9RrSNHWztMmapsj-e6u7iF4cGGYYPr5kmCw7BTQHxMklmyOgAog4yCYYWFkQjPnhr_44m_X9Go1BJaCSTrLyprUmxeDzLlSudWmbW7_S3tjO-pQ7n_viTj_lg69tzJerzpmis0m3J9lRo9vezvZ1mr3c3jwv7ovH5d3D4uqxMERCKqSGpsKGYJCVRqyWtmGUMs0wQ2XFMCeAKyFYIyiFSkLDiRSm4ZrWEleck2n2sPPWQa_VJrpOx60K2qnvQYhvSsfkTGuVAGDWWiwYYxRTImWJMB-fQyWSNSejq9i5-g-7Gao_tmv3evVta92gQApWypE_2_GbGN4H2ye1DkP047oKl4SMKTmM1PmOMjH0fbTNjxeQ-rqLYmp_l5G92P_AuKSTC_4f-BNK44fx</recordid><startdate>20230701</startdate><enddate>20230701</enddate><creator>Uryu, Kazuya</creator><creator>Deng, Yuchen</creator><creator>Le, Son Phuong</creator><creator>Suzuki, Toshi-kazu</creator><general>American Institute of Physics</general><general>AIP Publishing LLC</general><scope>AJDQP</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>ADTPV</scope><scope>AOWAS</scope><scope>DG8</scope><scope>DOA</scope><orcidid>https://orcid.org/0009-0000-5597-7853</orcidid><orcidid>https://orcid.org/0000-0001-9792-563X</orcidid><orcidid>https://orcid.org/0000-0003-4612-8299</orcidid><orcidid>https://orcid.org/0009-0009-6379-7313</orcidid></search><sort><creationdate>20230701</creationdate><title>Electron mobility enhancement in n-GaN under Ohmic-metal</title><author>Uryu, Kazuya ; Deng, Yuchen ; Le, Son Phuong ; Suzuki, Toshi-kazu</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c391t-9a1fb2c3219ba05d9ef5445a52508b526312b775f7441b91f6397cf6a4d92b663</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Annealing</topic><topic>Deposition</topic><topic>Doping</topic><topic>Electron density</topic><topic>Electron mobility</topic><topic>Electron transport</topic><topic>Gallium nitrides</topic><topic>Hall effect</topic><topic>High density</topic><topic>Impurities</topic><topic>Polarization</topic><topic>Scattering</topic><topic>Titanium</topic><topic>Transport properties</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Uryu, Kazuya</creatorcontrib><creatorcontrib>Deng, Yuchen</creatorcontrib><creatorcontrib>Le, Son Phuong</creatorcontrib><creatorcontrib>Suzuki, Toshi-kazu</creatorcontrib><collection>AIP Open Access Journals</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>SwePub</collection><collection>SwePub Articles</collection><collection>SWEPUB Linköpings universitet</collection><collection>DOAJ Directory of Open Access Journals</collection><jtitle>AIP advances</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Uryu, Kazuya</au><au>Deng, Yuchen</au><au>Le, Son Phuong</au><au>Suzuki, Toshi-kazu</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electron mobility enhancement in n-GaN under Ohmic-metal</atitle><jtitle>AIP advances</jtitle><date>2023-07-01</date><risdate>2023</risdate><volume>13</volume><issue>7</issue><spage>075002</spage><epage>075002-7</epage><pages>075002-075002-7</pages><issn>2158-3226</issn><eissn>2158-3226</eissn><coden>AAIDBI</coden><abstract>We investigated the electron transport properties of n-GaN under an Ohmic-metal. Hall measurement results were compared for n-GaN (A) before Ti-based metal deposition, (B) after Ti-based metal deposition but before annealing, (C) after Ohmic annealing, and (D) after Ohmic-metal removal, where multi-probe-Hall device measurements are required for (C), while the others, (A), (B), and (D), can be characterized by conventional Hall device measurements. The multi-probe-Hall device measurements for (C) elucidated that, under the Ohmic-metal, the electron concentration is increased and the electron mobility is enhanced in comparison with those for the other cases, (A), (B), and (D). The increased electron concentration indicates that high-density doping takes place in the n-GaN by the Ohmic annealing. However, the high-density doping is not observed after the Ohmic-metal removal. Moreover, the electron mobility enhancement under the Ohmic-metal cannot be explained by donor doping with ionized impurity scattering. These suggest that, under the Ohmic-metal, high-density donors are not formed, and high-density polarization doping owing to strain from the Ohmic-metal takes place. From theoretical calculations, we clarified that the increase in the electron density by polarization doping without donors leads to the suppression of ionized impurity scattering and consequently the electron mobility enhancement.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0147137</doi><tpages>7</tpages><orcidid>https://orcid.org/0009-0000-5597-7853</orcidid><orcidid>https://orcid.org/0000-0001-9792-563X</orcidid><orcidid>https://orcid.org/0000-0003-4612-8299</orcidid><orcidid>https://orcid.org/0009-0009-6379-7313</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Annealing Deposition Doping Electron density Electron mobility Electron transport Gallium nitrides Hall effect High density Impurities Polarization Scattering Titanium Transport properties |
title | Electron mobility enhancement in n-GaN under Ohmic-metal |
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