Distribution and transport of holes in the p-GaN/AlGaN/GaN heterostructure
The p-GaN/AlGaN/GaN heterostructure, predominantly epitaxially grown on large-scale silicon wafers, has been widely used for producing consumer power switching devices and recently manifested favorable for developing GaN-based complementary devices and circuits. This work investigates the hole distr...
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creator | Ng, Yat Hon Zheng, Zheyang Zhang, Li Liu, Ruizi Chen, Tao Feng, Sirui Shao, Qiming Chen, Kevin J. |
description | The p-GaN/AlGaN/GaN heterostructure, predominantly epitaxially grown on large-scale silicon wafers, has been widely used for producing consumer power switching devices and recently manifested favorable for developing GaN-based complementary devices and circuits. This work investigates the hole distribution and transport in this structure based on wide-temperature-range (20–600 K) Hall measurements and TCAD simulations. It is revealed that the p-channel thereof is composed of the bulk holes in the p-GaN and the two-dimensional hole gas (2DHG) at the p-GaN/AlGaN interface, and both substantially contribute to the lateral p-type conduction at room temperature. Their complementary temperature responses lead to conductivity enhancement at both high- and low-temperature regimes. The high-density (1.2 × 1013 cm−2) 2DHG is formed owing to the polarization-induced potential well and the ionization of the Mg acceptors that thermally diffused into the barrier during the epi-growth. Such ionized Mg acceptors would partially deplete the two-dimensional electron gas (2DEG) at the access region in the n-channel side where the p-GaN is removed and result in a trade-off between the carrier density of 2DHG and 2DEG. |
doi_str_mv | 10.1063/5.0172010 |
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This work investigates the hole distribution and transport in this structure based on wide-temperature-range (20–600 K) Hall measurements and TCAD simulations. It is revealed that the p-channel thereof is composed of the bulk holes in the p-GaN and the two-dimensional hole gas (2DHG) at the p-GaN/AlGaN interface, and both substantially contribute to the lateral p-type conduction at room temperature. Their complementary temperature responses lead to conductivity enhancement at both high- and low-temperature regimes. The high-density (1.2 × 1013 cm−2) 2DHG is formed owing to the polarization-induced potential well and the ionization of the Mg acceptors that thermally diffused into the barrier during the epi-growth. Such ionized Mg acceptors would partially deplete the two-dimensional electron gas (2DEG) at the access region in the n-channel side where the p-GaN is removed and result in a trade-off between the carrier density of 2DHG and 2DEG.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/5.0172010</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Aluminum gallium nitrides ; Applied physics ; Carrier density ; Conduction heating ; Diffusion barriers ; Electron gas ; Epitaxial growth ; Gallium nitrides ; Heterostructures ; Hole distribution ; Low temperature ; Power consumption ; Room temperature ; Silicon wafers</subject><ispartof>Applied physics letters, 2023-10, Vol.123 (14)</ispartof><rights>Author(s)</rights><rights>2023 Author(s). Published under an exclusive license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c292t-7dcb33fd329033fa9779151106701401d44506f524bf499ba49e60a274a6b7273</citedby><cites>FETCH-LOGICAL-c292t-7dcb33fd329033fa9779151106701401d44506f524bf499ba49e60a274a6b7273</cites><orcidid>0000-0003-2613-3031 ; 0000-0002-2127-3417 ; 0000-0003-2587-7936 ; 0000-0001-7400-6948 ; 0000-0002-6645-1096 ; 0000-0002-6455-9300 ; 0000-0002-0659-2022 ; 0000-0001-8402-0612</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/apl/article-lookup/doi/10.1063/5.0172010$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>315,781,785,795,4513,27929,27930,76389</link.rule.ids></links><search><creatorcontrib>Ng, Yat Hon</creatorcontrib><creatorcontrib>Zheng, Zheyang</creatorcontrib><creatorcontrib>Zhang, Li</creatorcontrib><creatorcontrib>Liu, Ruizi</creatorcontrib><creatorcontrib>Chen, Tao</creatorcontrib><creatorcontrib>Feng, Sirui</creatorcontrib><creatorcontrib>Shao, Qiming</creatorcontrib><creatorcontrib>Chen, Kevin J.</creatorcontrib><title>Distribution and transport of holes in the p-GaN/AlGaN/GaN heterostructure</title><title>Applied physics letters</title><description>The p-GaN/AlGaN/GaN heterostructure, predominantly epitaxially grown on large-scale silicon wafers, has been widely used for producing consumer power switching devices and recently manifested favorable for developing GaN-based complementary devices and circuits. This work investigates the hole distribution and transport in this structure based on wide-temperature-range (20–600 K) Hall measurements and TCAD simulations. It is revealed that the p-channel thereof is composed of the bulk holes in the p-GaN and the two-dimensional hole gas (2DHG) at the p-GaN/AlGaN interface, and both substantially contribute to the lateral p-type conduction at room temperature. Their complementary temperature responses lead to conductivity enhancement at both high- and low-temperature regimes. The high-density (1.2 × 1013 cm−2) 2DHG is formed owing to the polarization-induced potential well and the ionization of the Mg acceptors that thermally diffused into the barrier during the epi-growth. Such ionized Mg acceptors would partially deplete the two-dimensional electron gas (2DEG) at the access region in the n-channel side where the p-GaN is removed and result in a trade-off between the carrier density of 2DHG and 2DEG.</description><subject>Aluminum gallium nitrides</subject><subject>Applied physics</subject><subject>Carrier density</subject><subject>Conduction heating</subject><subject>Diffusion barriers</subject><subject>Electron gas</subject><subject>Epitaxial growth</subject><subject>Gallium nitrides</subject><subject>Heterostructures</subject><subject>Hole distribution</subject><subject>Low temperature</subject><subject>Power consumption</subject><subject>Room temperature</subject><subject>Silicon wafers</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kE9LAzEQxYMoWKsHv0HAk8K2M_mzaY6lalWKXvQcsrtZuqVu1iR78Nub0p49zDwGfjPzeITcIswQSj6XM0DFAOGMTBCUKjji4pxMAIAXpZZ4Sa5i3OVRMs4n5O2xiyl01Zg631PbNzQF28fBh0R9S7d-7yLtepq2jg7F2r7Pl_tDz0W3Lrng8_pYpzG4a3LR2n10Nyedkq_np8_VS7H5WL-ulpuiZpqlQjV1xXnbcKYhq9VKaZSY3StAAdgIIaFsJRNVK7SurNCuBMuUsGWlmOJTcne8OwT_M7qYzM6Poc8vDVsoJhjjmmXq_kjV2WIMrjVD6L5t-DUI5hCVkeYUVWYfjmysu2QPSfwD_wHRQGWq</recordid><startdate>20231002</startdate><enddate>20231002</enddate><creator>Ng, Yat Hon</creator><creator>Zheng, Zheyang</creator><creator>Zhang, Li</creator><creator>Liu, Ruizi</creator><creator>Chen, Tao</creator><creator>Feng, Sirui</creator><creator>Shao, Qiming</creator><creator>Chen, Kevin J.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-2613-3031</orcidid><orcidid>https://orcid.org/0000-0002-2127-3417</orcidid><orcidid>https://orcid.org/0000-0003-2587-7936</orcidid><orcidid>https://orcid.org/0000-0001-7400-6948</orcidid><orcidid>https://orcid.org/0000-0002-6645-1096</orcidid><orcidid>https://orcid.org/0000-0002-6455-9300</orcidid><orcidid>https://orcid.org/0000-0002-0659-2022</orcidid><orcidid>https://orcid.org/0000-0001-8402-0612</orcidid></search><sort><creationdate>20231002</creationdate><title>Distribution and transport of holes in the p-GaN/AlGaN/GaN heterostructure</title><author>Ng, Yat Hon ; Zheng, Zheyang ; Zhang, Li ; Liu, Ruizi ; Chen, Tao ; Feng, Sirui ; Shao, Qiming ; Chen, Kevin J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c292t-7dcb33fd329033fa9779151106701401d44506f524bf499ba49e60a274a6b7273</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Aluminum gallium nitrides</topic><topic>Applied physics</topic><topic>Carrier density</topic><topic>Conduction heating</topic><topic>Diffusion barriers</topic><topic>Electron gas</topic><topic>Epitaxial growth</topic><topic>Gallium nitrides</topic><topic>Heterostructures</topic><topic>Hole distribution</topic><topic>Low temperature</topic><topic>Power consumption</topic><topic>Room temperature</topic><topic>Silicon wafers</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ng, Yat Hon</creatorcontrib><creatorcontrib>Zheng, Zheyang</creatorcontrib><creatorcontrib>Zhang, Li</creatorcontrib><creatorcontrib>Liu, Ruizi</creatorcontrib><creatorcontrib>Chen, Tao</creatorcontrib><creatorcontrib>Feng, Sirui</creatorcontrib><creatorcontrib>Shao, Qiming</creatorcontrib><creatorcontrib>Chen, Kevin J.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ng, Yat Hon</au><au>Zheng, Zheyang</au><au>Zhang, Li</au><au>Liu, Ruizi</au><au>Chen, Tao</au><au>Feng, Sirui</au><au>Shao, Qiming</au><au>Chen, Kevin J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Distribution and transport of holes in the p-GaN/AlGaN/GaN heterostructure</atitle><jtitle>Applied physics letters</jtitle><date>2023-10-02</date><risdate>2023</risdate><volume>123</volume><issue>14</issue><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>The p-GaN/AlGaN/GaN heterostructure, predominantly epitaxially grown on large-scale silicon wafers, has been widely used for producing consumer power switching devices and recently manifested favorable for developing GaN-based complementary devices and circuits. This work investigates the hole distribution and transport in this structure based on wide-temperature-range (20–600 K) Hall measurements and TCAD simulations. It is revealed that the p-channel thereof is composed of the bulk holes in the p-GaN and the two-dimensional hole gas (2DHG) at the p-GaN/AlGaN interface, and both substantially contribute to the lateral p-type conduction at room temperature. Their complementary temperature responses lead to conductivity enhancement at both high- and low-temperature regimes. The high-density (1.2 × 1013 cm−2) 2DHG is formed owing to the polarization-induced potential well and the ionization of the Mg acceptors that thermally diffused into the barrier during the epi-growth. Such ionized Mg acceptors would partially deplete the two-dimensional electron gas (2DEG) at the access region in the n-channel side where the p-GaN is removed and result in a trade-off between the carrier density of 2DHG and 2DEG.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0172010</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0003-2613-3031</orcidid><orcidid>https://orcid.org/0000-0002-2127-3417</orcidid><orcidid>https://orcid.org/0000-0003-2587-7936</orcidid><orcidid>https://orcid.org/0000-0001-7400-6948</orcidid><orcidid>https://orcid.org/0000-0002-6645-1096</orcidid><orcidid>https://orcid.org/0000-0002-6455-9300</orcidid><orcidid>https://orcid.org/0000-0002-0659-2022</orcidid><orcidid>https://orcid.org/0000-0001-8402-0612</orcidid></addata></record> |
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subjects | Aluminum gallium nitrides Applied physics Carrier density Conduction heating Diffusion barriers Electron gas Epitaxial growth Gallium nitrides Heterostructures Hole distribution Low temperature Power consumption Room temperature Silicon wafers |
title | Distribution and transport of holes in the p-GaN/AlGaN/GaN heterostructure |
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