Yunfei Niu, Gaoqiang Deng*, Tao Wang, Haotian Ma, Shixu Yang, Jiaqi Yu, Lidong Zhang, Yusen Wang, Changcai Zuo, Bin Duan, Baolin Zhang, Guoxing Li, Xiaojuan Sun, Dabing Li and Yuantao Zhang*,
{"title":"利用晶格极性操纵碳化硅基板上的氮化铝薄膜,制造 N 极氮化镓 HEMT","authors":"Yunfei Niu, Gaoqiang Deng*, Tao Wang, Haotian Ma, Shixu Yang, Jiaqi Yu, Lidong Zhang, Yusen Wang, Changcai Zuo, Bin Duan, Baolin Zhang, Guoxing Li, Xiaojuan Sun, Dabing Li and Yuantao Zhang*, ","doi":"10.1021/acs.cgd.4c0058510.1021/acs.cgd.4c00585","DOIUrl":null,"url":null,"abstract":"<p >Realization of nitrogen-polar (N-polar) AlN on SiC is important for the development of high-performance GaN high-electron mobility transistors (HEMTs). However, AlN films grown on SiC substrates are mostly metal-polar, and it is difficult to achieve an N-polar AlN on them. In this work, we manipulated the lattice polarity of AlN grown on SiC by varying the V/III ratio. Our results show that AlN films grown at a low V/III ratio undergo lattice polarity reversal from N-polarity to metal-polarity near the AlN/SiC interface. This occurs because oxygen enrichment occurs in AlN, forming a thin AlON layer close to the interface. Importantly, we suppress the oxygen enrichment and thus the formation of AlON in AlN under a high V/III ratio, i.e., an N-rich growth condition, and finally achieve an N-polar AlN film on SiC. We also find that the threshold V/III ratio that realizes N-polar AlN on SiC without lattice polarity reversal is ∼6000. Furthermore, we prepared a GaN/AlGaN HEMT structure based on the obtained N-polar AlN, and the 2-dimensional electron gas density and mobility at the heterostructure interface are 1.5 × 10<sup>13</sup> cm<sup>–2</sup> and 923 cm<sup>2</sup>/V·s, respectively. This work is expected to promote the development of N-polar GaN HEMTs on SiC.</p>","PeriodicalId":3,"journal":{"name":"ACS Applied Electronic Materials","volume":null,"pages":null},"PeriodicalIF":4.3000,"publicationDate":"2024-08-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Lattice Polarity Manipulation of AlN Films on SiC Substrates for N-Polar GaN HEMTs\",\"authors\":\"Yunfei Niu, Gaoqiang Deng*, Tao Wang, Haotian Ma, Shixu Yang, Jiaqi Yu, Lidong Zhang, Yusen Wang, Changcai Zuo, Bin Duan, Baolin Zhang, Guoxing Li, Xiaojuan Sun, Dabing Li and Yuantao Zhang*, \",\"doi\":\"10.1021/acs.cgd.4c0058510.1021/acs.cgd.4c00585\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >Realization of nitrogen-polar (N-polar) AlN on SiC is important for the development of high-performance GaN high-electron mobility transistors (HEMTs). However, AlN films grown on SiC substrates are mostly metal-polar, and it is difficult to achieve an N-polar AlN on them. In this work, we manipulated the lattice polarity of AlN grown on SiC by varying the V/III ratio. Our results show that AlN films grown at a low V/III ratio undergo lattice polarity reversal from N-polarity to metal-polarity near the AlN/SiC interface. This occurs because oxygen enrichment occurs in AlN, forming a thin AlON layer close to the interface. Importantly, we suppress the oxygen enrichment and thus the formation of AlON in AlN under a high V/III ratio, i.e., an N-rich growth condition, and finally achieve an N-polar AlN film on SiC. We also find that the threshold V/III ratio that realizes N-polar AlN on SiC without lattice polarity reversal is ∼6000. Furthermore, we prepared a GaN/AlGaN HEMT structure based on the obtained N-polar AlN, and the 2-dimensional electron gas density and mobility at the heterostructure interface are 1.5 × 10<sup>13</sup> cm<sup>–2</sup> and 923 cm<sup>2</sup>/V·s, respectively. This work is expected to promote the development of N-polar GaN HEMTs on SiC.</p>\",\"PeriodicalId\":3,\"journal\":{\"name\":\"ACS Applied Electronic Materials\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":4.3000,\"publicationDate\":\"2024-08-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ACS Applied Electronic Materials\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://pubs.acs.org/doi/10.1021/acs.cgd.4c00585\",\"RegionNum\":3,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Electronic Materials","FirstCategoryId":"92","ListUrlMain":"https://pubs.acs.org/doi/10.1021/acs.cgd.4c00585","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
摘要
在碳化硅(SiC)上实现氮极性(N-polar)AlN 对于开发高性能氮化镓高电子迁移率晶体管(HEMT)非常重要。然而,在碳化硅衬底上生长的 AlN 薄膜大多是金属极性的,因此很难在其上实现氮极性 AlN。在这项工作中,我们通过改变 V/III 的比例来操纵在 SiC 上生长的 AlN 的晶格极性。我们的研究结果表明,以低 V/III 比率生长的 AlN 薄膜在 AlN/SiC 界面附近会发生晶格极性反转,从 N 极性转变为金属极性。出现这种情况的原因是 AlN 中出现了氧富集,在靠近界面的地方形成了一层薄薄的 AlON 层。重要的是,在高 V/III 比(即富含 N 的生长条件)下,我们抑制了 AlN 中的氧富集,从而抑制了 AlON 的形成,最终在 SiC 上形成了 N 极 AlN 薄膜。我们还发现,在 SiC 上实现无晶格极性反转的 N 极 AlN 的阈值 V/III 比为 ∼ 6000。此外,我们基于所获得的 N 极 AlN 制备了 GaN/AlGaN HEMT 结构,异质结构界面上的二维电子气体密度和迁移率分别为 1.5 × 1013 cm-2 和 923 cm2/V-s。这项工作有望推动氮化镓 HEMT 在碳化硅上的发展。
Lattice Polarity Manipulation of AlN Films on SiC Substrates for N-Polar GaN HEMTs
Realization of nitrogen-polar (N-polar) AlN on SiC is important for the development of high-performance GaN high-electron mobility transistors (HEMTs). However, AlN films grown on SiC substrates are mostly metal-polar, and it is difficult to achieve an N-polar AlN on them. In this work, we manipulated the lattice polarity of AlN grown on SiC by varying the V/III ratio. Our results show that AlN films grown at a low V/III ratio undergo lattice polarity reversal from N-polarity to metal-polarity near the AlN/SiC interface. This occurs because oxygen enrichment occurs in AlN, forming a thin AlON layer close to the interface. Importantly, we suppress the oxygen enrichment and thus the formation of AlON in AlN under a high V/III ratio, i.e., an N-rich growth condition, and finally achieve an N-polar AlN film on SiC. We also find that the threshold V/III ratio that realizes N-polar AlN on SiC without lattice polarity reversal is ∼6000. Furthermore, we prepared a GaN/AlGaN HEMT structure based on the obtained N-polar AlN, and the 2-dimensional electron gas density and mobility at the heterostructure interface are 1.5 × 1013 cm–2 and 923 cm2/V·s, respectively. This work is expected to promote the development of N-polar GaN HEMTs on SiC.