用于 275 纳米深紫外发光二极管的偏振掺杂 AlxGa1-xN(x = 0.9-0.35)- 梯度层中的空穴生成,带高镁掺杂 Al0.35Ga0.65N 接触层

Hayata Takahata, Tomoaki Kachi, Naoki Hamashima, Ryunosuke Oka, Hisanori Ishiguro, Tetsuya Takeuchi, S. Kamiyama, M. Iwaya, Y. Saito, K. Okuno
{"title":"用于 275 纳米深紫外发光二极管的偏振掺杂 AlxGa1-xN(x = 0.9-0.35)- 梯度层中的空穴生成,带高镁掺杂 Al0.35Ga0.65N 接触层","authors":"Hayata Takahata, Tomoaki Kachi, Naoki Hamashima, Ryunosuke Oka, Hisanori Ishiguro, Tetsuya Takeuchi, S. Kamiyama, M. Iwaya, Y. Saito, K. Okuno","doi":"10.1002/pssa.202400054","DOIUrl":null,"url":null,"abstract":"Herein, hole generation in a 60 nm thick polarization‐doped AlxGa1–xN (x = 0.9–0.35)‐graded layer with some Mg doping (5 × 1018 cm−3) is demonstrated by using a 10 nm thick heavily (1 × 1020 cm−3) Mg‐doped Al0.35Ga0.65N contact layer. First, light emission from a deep‐ultraviolet light‐emitting diode is observed with the AlxGa1–xN (x = 0.9–0.35)‐graded layer and the Al0.35Ga0.65N contact layer, indicating a vertical hole transport from the Al0.35Ga0.65N contact layer to the active region through the polarization‐doped AlGaN‐graded layer. Second, hole concentration, mobility, and resistivity values of the AlxGa1–xN (x = 0.9–0.35)‐graded layer and the Al0.35Ga0.65N contact layer are evaluated by Hall effect measurement. A hole concentration of 1.8 × 1018 cm−3 is clearly observed by removing the AlGaN contact layer (not underneath of electrodes) to minimize a parallel conduction. The hole concentration shows a very weak temperature dependence from room temperature down to 150 K, suggesting that the holes are generated by polarization doping. Hole generation in the fully strained AlxGa1–xN (x = 0.9–0.35)‐graded layer is directly evaluated by Hall effect measurement with the AlGaN contact layer just underneath the electrodes.","PeriodicalId":20150,"journal":{"name":"physica status solidi (a)","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Hole Generation in Polarization‐Doped AlxGa1–xN (x = 0.9–0.35)‐Graded Layer with Heavily Mg‐Doped Al0.35Ga0.65N Contact Layer for 275 nm Deep‐Ultraviolet Light‐Emitting Diode\",\"authors\":\"Hayata Takahata, Tomoaki Kachi, Naoki Hamashima, Ryunosuke Oka, Hisanori Ishiguro, Tetsuya Takeuchi, S. Kamiyama, M. Iwaya, Y. Saito, K. Okuno\",\"doi\":\"10.1002/pssa.202400054\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Herein, hole generation in a 60 nm thick polarization‐doped AlxGa1–xN (x = 0.9–0.35)‐graded layer with some Mg doping (5 × 1018 cm−3) is demonstrated by using a 10 nm thick heavily (1 × 1020 cm−3) Mg‐doped Al0.35Ga0.65N contact layer. First, light emission from a deep‐ultraviolet light‐emitting diode is observed with the AlxGa1–xN (x = 0.9–0.35)‐graded layer and the Al0.35Ga0.65N contact layer, indicating a vertical hole transport from the Al0.35Ga0.65N contact layer to the active region through the polarization‐doped AlGaN‐graded layer. Second, hole concentration, mobility, and resistivity values of the AlxGa1–xN (x = 0.9–0.35)‐graded layer and the Al0.35Ga0.65N contact layer are evaluated by Hall effect measurement. A hole concentration of 1.8 × 1018 cm−3 is clearly observed by removing the AlGaN contact layer (not underneath of electrodes) to minimize a parallel conduction. The hole concentration shows a very weak temperature dependence from room temperature down to 150 K, suggesting that the holes are generated by polarization doping. Hole generation in the fully strained AlxGa1–xN (x = 0.9–0.35)‐graded layer is directly evaluated by Hall effect measurement with the AlGaN contact layer just underneath the electrodes.\",\"PeriodicalId\":20150,\"journal\":{\"name\":\"physica status solidi (a)\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-06-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"physica status solidi (a)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1002/pssa.202400054\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"physica status solidi (a)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1002/pssa.202400054","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

摘要

在此,通过使用 10 nm 厚(1 × 1020 cm-3)的大量掺入镁的 Al0.35Ga0.65N 接触层,演示了在 60 nm 厚的偏振掺杂 AlxGa1-xN (x = 0.9-0.35)分级层中产生空穴的过程。首先,在 AlxGa1-xN(x = 0.9-0.35)分级层和 Al0.35Ga0.65N 接触层上观察到了深紫外发光二极管的光发射,表明空穴从 Al0.35Ga0.65N 接触层通过极化掺杂的 AlGaN 分级层垂直传输到有源区。其次,通过霍尔效应测量评估了 AlxGa1-xN(x = 0.9-0.35)分级层和 Al0.35Ga0.65N 接触层的空穴浓度、迁移率和电阻率值。通过移除 AlGaN 接触层(非电极下方)以减少平行传导,可以清楚地观察到 1.8 × 1018 cm-3 的空穴浓度。从室温到 150 K,空穴浓度与温度的关系非常微弱,这表明空穴是通过极化掺杂产生的。通过霍尔效应测量直接评估了完全应变的 AlxGa1-xN (x = 0.9-0.35) 梯度层中的空穴生成情况,AlGaN 接触层正好位于电极下方。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Hole Generation in Polarization‐Doped AlxGa1–xN (x = 0.9–0.35)‐Graded Layer with Heavily Mg‐Doped Al0.35Ga0.65N Contact Layer for 275 nm Deep‐Ultraviolet Light‐Emitting Diode
Herein, hole generation in a 60 nm thick polarization‐doped AlxGa1–xN (x = 0.9–0.35)‐graded layer with some Mg doping (5 × 1018 cm−3) is demonstrated by using a 10 nm thick heavily (1 × 1020 cm−3) Mg‐doped Al0.35Ga0.65N contact layer. First, light emission from a deep‐ultraviolet light‐emitting diode is observed with the AlxGa1–xN (x = 0.9–0.35)‐graded layer and the Al0.35Ga0.65N contact layer, indicating a vertical hole transport from the Al0.35Ga0.65N contact layer to the active region through the polarization‐doped AlGaN‐graded layer. Second, hole concentration, mobility, and resistivity values of the AlxGa1–xN (x = 0.9–0.35)‐graded layer and the Al0.35Ga0.65N contact layer are evaluated by Hall effect measurement. A hole concentration of 1.8 × 1018 cm−3 is clearly observed by removing the AlGaN contact layer (not underneath of electrodes) to minimize a parallel conduction. The hole concentration shows a very weak temperature dependence from room temperature down to 150 K, suggesting that the holes are generated by polarization doping. Hole generation in the fully strained AlxGa1–xN (x = 0.9–0.35)‐graded layer is directly evaluated by Hall effect measurement with the AlGaN contact layer just underneath the electrodes.
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
自引率
0.00%
发文量
0
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信