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":"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}
引用次数: 0
Abstract
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.