{"title":"用于带隙调制的 N 掺杂氧化镓薄膜的等离子体增强原子层沉积","authors":"Longxing Su , Hongping Ma","doi":"10.1016/j.tsf.2024.140561","DOIUrl":null,"url":null,"abstract":"<div><div>Bandgap modulation is extremely important for optoelectronic and electronic devices. However, compare with Ⅱ-Ⅵ and Ⅲ-Ⅴ compound semiconductors, the ultrawide bandgap semiconductor Ga<sub>2</sub>O<sub>3</sub> (Ⅲ-Ⅵ) faces a tough obstacle of bandgap modulation. Herein, we have prepared a N-doped GaO thin film on Si substrate through a plasma-enhanced atomic layer deposition (PEALD) method. The as-deposited GaO:N layer exhibits amorphous nature with thickness of ∼8.4 nm. The bandgap of the as-deposited GaO:N layer is adjusted to 4.31 eV, which is ∼0.49 eV smaller than the bandgap of pure Ga<sub>2</sub>O<sub>3</sub>. In addition, the photoluminescence (PL) spectra from five randomly selected points of the film layer indicate the uniformly distribution of N concentration. Subsequently, the energy band diagram of the as-deposited GaO:N layer is determined by the X-ray photoelectron spectroscopy (XPS), in which the Fermi energy level locates ∼0.81 eV below the conduction band minimum (CBM) and ∼3.5 eV above the valence band maximum (VBM). Our study raises a promising strategy for modulating the bandgap of Ga<sub>2</sub>O<sub>3</sub>, which provides potential applications in spectrum adjustable photodetector and high electron mobility transistor.</div></div>","PeriodicalId":23182,"journal":{"name":"Thin Solid Films","volume":"808 ","pages":"Article 140561"},"PeriodicalIF":2.0000,"publicationDate":"2024-10-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Plasma-enhanced atomic layer deposition of N-doped GaO thin film for bandgap modulation\",\"authors\":\"Longxing Su , Hongping Ma\",\"doi\":\"10.1016/j.tsf.2024.140561\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Bandgap modulation is extremely important for optoelectronic and electronic devices. However, compare with Ⅱ-Ⅵ and Ⅲ-Ⅴ compound semiconductors, the ultrawide bandgap semiconductor Ga<sub>2</sub>O<sub>3</sub> (Ⅲ-Ⅵ) faces a tough obstacle of bandgap modulation. Herein, we have prepared a N-doped GaO thin film on Si substrate through a plasma-enhanced atomic layer deposition (PEALD) method. The as-deposited GaO:N layer exhibits amorphous nature with thickness of ∼8.4 nm. The bandgap of the as-deposited GaO:N layer is adjusted to 4.31 eV, which is ∼0.49 eV smaller than the bandgap of pure Ga<sub>2</sub>O<sub>3</sub>. In addition, the photoluminescence (PL) spectra from five randomly selected points of the film layer indicate the uniformly distribution of N concentration. Subsequently, the energy band diagram of the as-deposited GaO:N layer is determined by the X-ray photoelectron spectroscopy (XPS), in which the Fermi energy level locates ∼0.81 eV below the conduction band minimum (CBM) and ∼3.5 eV above the valence band maximum (VBM). Our study raises a promising strategy for modulating the bandgap of Ga<sub>2</sub>O<sub>3</sub>, which provides potential applications in spectrum adjustable photodetector and high electron mobility transistor.</div></div>\",\"PeriodicalId\":23182,\"journal\":{\"name\":\"Thin Solid Films\",\"volume\":\"808 \",\"pages\":\"Article 140561\"},\"PeriodicalIF\":2.0000,\"publicationDate\":\"2024-10-28\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Thin Solid Films\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0040609024003626\",\"RegionNum\":4,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"MATERIALS SCIENCE, COATINGS & FILMS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Thin Solid Films","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0040609024003626","RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"MATERIALS SCIENCE, COATINGS & FILMS","Score":null,"Total":0}
引用次数: 0
摘要
带隙调制对光电和电子设备极为重要。然而,与Ⅱ-Ⅵ和Ⅲ-Ⅴ化合物半导体相比,超宽带隙半导体 Ga2O3(Ⅲ-Ⅵ)在带隙调制方面面临着严峻的挑战。在此,我们采用等离子体增强原子层沉积(PEALD)方法在硅衬底上制备了掺杂 N 的 GaO 薄膜。沉积后的 GaO:N 层呈非晶态,厚度为 8.4 nm。所沉积的 GaO:N 层的带隙被调整为 4.31 eV,比纯 Ga2O3 的带隙小 0.49 eV。此外,从薄膜层上随机选取的五个点的光致发光(PL)光谱显示出 N 浓度的均匀分布。随后,通过 X 射线光电子能谱(XPS)测定了淀积的 GaO:N 层的能带图,其中费米能级位于导带最小值(CBM)下方 ∼0.81 eV 和价带最大值(VBM)上方 ∼3.5 eV。我们的研究为调控 Ga2O3 的带隙提出了一种有前途的策略,为光谱可调光电探测器和高电子迁移率晶体管提供了潜在的应用。
Plasma-enhanced atomic layer deposition of N-doped GaO thin film for bandgap modulation
Bandgap modulation is extremely important for optoelectronic and electronic devices. However, compare with Ⅱ-Ⅵ and Ⅲ-Ⅴ compound semiconductors, the ultrawide bandgap semiconductor Ga2O3 (Ⅲ-Ⅵ) faces a tough obstacle of bandgap modulation. Herein, we have prepared a N-doped GaO thin film on Si substrate through a plasma-enhanced atomic layer deposition (PEALD) method. The as-deposited GaO:N layer exhibits amorphous nature with thickness of ∼8.4 nm. The bandgap of the as-deposited GaO:N layer is adjusted to 4.31 eV, which is ∼0.49 eV smaller than the bandgap of pure Ga2O3. In addition, the photoluminescence (PL) spectra from five randomly selected points of the film layer indicate the uniformly distribution of N concentration. Subsequently, the energy band diagram of the as-deposited GaO:N layer is determined by the X-ray photoelectron spectroscopy (XPS), in which the Fermi energy level locates ∼0.81 eV below the conduction band minimum (CBM) and ∼3.5 eV above the valence band maximum (VBM). Our study raises a promising strategy for modulating the bandgap of Ga2O3, which provides potential applications in spectrum adjustable photodetector and high electron mobility transistor.
期刊介绍:
Thin Solid Films is an international journal which serves scientists and engineers working in the fields of thin-film synthesis, characterization, and applications. The field of thin films, which can be defined as the confluence of materials science, surface science, and applied physics, has become an identifiable unified discipline of scientific endeavor.