{"title":"铑合金β氧化镓材料:新型三元超宽带隙半导体","authors":"Xian-Hu Zha, Yu-Xi Wan, Shuang Li, Dao Hua Zhang","doi":"10.1002/aelm.202400547","DOIUrl":null,"url":null,"abstract":"Beta gallium oxide (<i>β</i>-Ga<sub>2</sub>O<sub>3</sub>) is an ultra-wide-bandgap semiconductor with advantages for high-power electronics. However, the power resistance of <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>-based devices is still much lower than its material limit due to its flat band dispersion at its valence band maximum (VBM) and the difficulty for <i>p</i>-type doping. Here, <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>-based new type ternary ultra-wide bandgap semiconductors: <i>β</i>-(Rh<i><sub>x</sub></i>Ga<i><sub>1-x</sub></i>)<sub>2</sub>O<sub>3</sub>’s alloys are reported with <i>x</i> up to 0.5. The energy and band-dispersion curvature of <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>’s VBM are significantly enhanced via Rh-alloying. Compared to that in <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>, the <i>β</i>-(Rh<i><sub>x</sub></i>Ga<i><sub>1-x</sub></i>)<sub>2</sub>O<sub>3</sub>’s VBMs increase more than 1.35 <i>eV</i>. The hole mass of <i>β</i>-(Rh<sub>0.25</sub>Ga<sub>0.75</sub>)<sub>2</sub>O<sub>3</sub> is only 52.3% of that in <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>. The decreased hole mass is correlated with the equal Rh─O bond along the <i>b</i>-axis. Thanks to the simultaneous rise of conduction band minimums, the bandgaps of <i>β</i>-(Rh<i><sub>x</sub></i>Ga<i><sub>1-x</sub></i>)<sub>2</sub>O<sub>3</sub> are still much larger than that in commercial silicon carbide. Moreover, the alloys show direct bandgaps in a wide range of <i>x</i>, and a direct and ultra-wide bandgap of 4.10 <i>eV</i> is determined in <i>β</i>-(Rh<sub>0.3125</sub>Ga<sub>0.6875</sub>)<sub>2</sub>O<sub>3</sub>. Combined with the enhanced valence energy, reduced hole mass, and ultra-wide bandgap, the <i>β</i>-(Rh<i><sub>x</sub></i>Ga<i><sub>1-x</sub></i>)<sub>2</sub>O<sub>3</sub> can be candidate semiconductors for a new generation of power electronics, ultraviolet optoelectronics, and complementary metal-oxide-semiconductor (CMOS) technologies.","PeriodicalId":110,"journal":{"name":"Advanced Electronic Materials","volume":"24 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2024-10-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Rhodium-Alloyed Beta Gallium Oxide Materials: New Type Ternary Ultra-Wide Bandgap Semiconductors\",\"authors\":\"Xian-Hu Zha, Yu-Xi Wan, Shuang Li, Dao Hua Zhang\",\"doi\":\"10.1002/aelm.202400547\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Beta gallium oxide (<i>β</i>-Ga<sub>2</sub>O<sub>3</sub>) is an ultra-wide-bandgap semiconductor with advantages for high-power electronics. However, the power resistance of <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>-based devices is still much lower than its material limit due to its flat band dispersion at its valence band maximum (VBM) and the difficulty for <i>p</i>-type doping. Here, <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>-based new type ternary ultra-wide bandgap semiconductors: <i>β</i>-(Rh<i><sub>x</sub></i>Ga<i><sub>1-x</sub></i>)<sub>2</sub>O<sub>3</sub>’s alloys are reported with <i>x</i> up to 0.5. The energy and band-dispersion curvature of <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>’s VBM are significantly enhanced via Rh-alloying. Compared to that in <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>, the <i>β</i>-(Rh<i><sub>x</sub></i>Ga<i><sub>1-x</sub></i>)<sub>2</sub>O<sub>3</sub>’s VBMs increase more than 1.35 <i>eV</i>. The hole mass of <i>β</i>-(Rh<sub>0.25</sub>Ga<sub>0.75</sub>)<sub>2</sub>O<sub>3</sub> is only 52.3% of that in <i>β</i>-Ga<sub>2</sub>O<sub>3</sub>. The decreased hole mass is correlated with the equal Rh─O bond along the <i>b</i>-axis. Thanks to the simultaneous rise of conduction band minimums, the bandgaps of <i>β</i>-(Rh<i><sub>x</sub></i>Ga<i><sub>1-x</sub></i>)<sub>2</sub>O<sub>3</sub> are still much larger than that in commercial silicon carbide. Moreover, the alloys show direct bandgaps in a wide range of <i>x</i>, and a direct and ultra-wide bandgap of 4.10 <i>eV</i> is determined in <i>β</i>-(Rh<sub>0.3125</sub>Ga<sub>0.6875</sub>)<sub>2</sub>O<sub>3</sub>. Combined with the enhanced valence energy, reduced hole mass, and ultra-wide bandgap, the <i>β</i>-(Rh<i><sub>x</sub></i>Ga<i><sub>1-x</sub></i>)<sub>2</sub>O<sub>3</sub> can be candidate semiconductors for a new generation of power electronics, ultraviolet optoelectronics, and complementary metal-oxide-semiconductor (CMOS) technologies.\",\"PeriodicalId\":110,\"journal\":{\"name\":\"Advanced Electronic Materials\",\"volume\":\"24 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2024-10-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advanced Electronic Materials\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://doi.org/10.1002/aelm.202400547\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Electronic Materials","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1002/aelm.202400547","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
β-氧化镓(β-Ga2O3)是一种超宽带隙半导体,具有大功率电子器件的优势。然而,由于β-Ga2O3 在价带最大值(VBM)处的平坦带色散以及难以进行 p 型掺杂,其器件的功率电阻仍远低于其材料极限。在此,我们将介绍基于 β-Ga2O3 的新型三元超宽带隙半导体:β-(RhxGa1-x)2O3合金。通过 Rh-合金化,β-Ga2O3 的 VBM 能量和带散曲率显著提高。与 β-Ga2O3 相比,β-(RhxGa1-x)2O3 的 VBM 增加了 1.35 eV 以上。β-(Rh0.25Ga0.75)2O3的空穴质量仅为β-Ga2O3的52.3%。空穴质量的减少与沿 b 轴的 Rh─O 键相等有关。由于导带最小值同时上升,β-(RhxGa1-x)2O3 的带隙仍然比商用碳化硅的带隙大得多。此外,这些合金在很宽的 x 范围内显示出直接带隙,在 β-(Rh0.3125Ga0.6875)2O3 中确定了 4.10 eV 的直接超宽带隙。结合增强的价能、降低的空穴质量和超宽带隙,β-(RhxGa1-x)2O3 可以成为新一代电力电子、紫外光电子和互补金属氧化物半导体(CMOS)技术的候选半导体。
Rhodium-Alloyed Beta Gallium Oxide Materials: New Type Ternary Ultra-Wide Bandgap Semiconductors
Beta gallium oxide (β-Ga2O3) is an ultra-wide-bandgap semiconductor with advantages for high-power electronics. However, the power resistance of β-Ga2O3-based devices is still much lower than its material limit due to its flat band dispersion at its valence band maximum (VBM) and the difficulty for p-type doping. Here, β-Ga2O3-based new type ternary ultra-wide bandgap semiconductors: β-(RhxGa1-x)2O3’s alloys are reported with x up to 0.5. The energy and band-dispersion curvature of β-Ga2O3’s VBM are significantly enhanced via Rh-alloying. Compared to that in β-Ga2O3, the β-(RhxGa1-x)2O3’s VBMs increase more than 1.35 eV. The hole mass of β-(Rh0.25Ga0.75)2O3 is only 52.3% of that in β-Ga2O3. The decreased hole mass is correlated with the equal Rh─O bond along the b-axis. Thanks to the simultaneous rise of conduction band minimums, the bandgaps of β-(RhxGa1-x)2O3 are still much larger than that in commercial silicon carbide. Moreover, the alloys show direct bandgaps in a wide range of x, and a direct and ultra-wide bandgap of 4.10 eV is determined in β-(Rh0.3125Ga0.6875)2O3. Combined with the enhanced valence energy, reduced hole mass, and ultra-wide bandgap, the β-(RhxGa1-x)2O3 can be candidate semiconductors for a new generation of power electronics, ultraviolet optoelectronics, and complementary metal-oxide-semiconductor (CMOS) technologies.
期刊介绍:
Advanced Electronic Materials is an interdisciplinary forum for peer-reviewed, high-quality, high-impact research in the fields of materials science, physics, and engineering of electronic and magnetic materials. It includes research on physics and physical properties of electronic and magnetic materials, spintronics, electronics, device physics and engineering, micro- and nano-electromechanical systems, and organic electronics, in addition to fundamental research.