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通过电调控和层间耦合调控石墨烯基范德华异质结构的电子性质与肖特基接触

Tuning electronic properties and Schottky contact in graphene-based van der Waals heterostructures by electric gating and interlayer coupling

Poonam Sharma, Archana Sharma, Alok Shukla

arXiv 2608.16413首次发表:更新:

AI 中文总结

本研究通过第一性原理计算,探究三种石墨烯基二维范德华异质结构,利用电调控和层间耦合可调控其肖特基接触类型、能带排列,还分析了光学响应与激子结合能,为相关器件设计提供理论依据。

AI 中文摘要

包含石墨烯(GE)的范德华异质结构(vdW HTSs)因具备制备出多种应用器件的潜力,成为理论与实验研究的活跃领域。本文采用第一性原理计算,研究了C₆N₆/GE、hg-C₃N₄/GE和C₆N₆/hg-C₃N₄这三种二维范德华异质结构,系统分析了半导体/金属及半导体/半导体界面的结构与热力学稳定性、电子性质、力学性质和光学性质。两种半导体/金属异质结构均形成n型肖特基接触,通过调控外加垂直电场和层间耦合,可将其转化为p型肖特基接触或欧姆接触。在半导体/半导体C₆N₆/hg-C₃N₄异质结构中,价带顶和导带底源自不同层,形成II型能带排列,可促进高效的电子-空穴(e-h)分离;外加电场和改变层间距,能有效将其能带排列在I型与II型之间调控。从异质结构的光吸收光谱可知,C₆N₆/GE和hg-C₃N₄/GE在宽频率范围内表现出光学响应,而C₆N₆/hg-C₃N₄异质结构主要在紫外区有显著活性。采用G₀W₀+BSE方法,计算了带隙体系(即C₆N₆单层、hg-C₃N₄单层及其异质结构C₆N₆/hg-C₃N₄)的激子结合能,分别为1.01 eV、1.14 eV和1.18 eV,凸显出强电子-空穴相互作用;此外,C₆N₆/hg-C₃N₄异质结构的带边分析进一步表明其有利于显著的层间电子-空穴耦合。

英文摘要

Van der Waals heterostructures (vdW HTSs) incorporating graphene (GE) have been an active area of research, both theoretical and experimental, due to their potential to yield devices with a wide variety of applications. In this paper, first-principles calculations are employed to investigate C$_{6}$N$_{6}$/GE, hg-C$_{3}$N$_{4}$/GE, and C$_{6}$N$_{6}$/hg-C$_{3}$N$_{4}$ 2D vdW HTSs. A systematic analysis of structural and thermodynamic stability, electronic, mechanical, and optical properties of semiconductor/metal and semiconductor/semiconductor interfaces is performed. Both semiconductor/metal HTSs form $n$-type Schottky contacts, which can be converted into $p$-type Schottky or Ohmic contacts by tuning the external perpendicular electric field and the interlayer coupling. In the semiconductor/semiconductor C$_{6}$N$_{6}$/hg-C$_{3}$N$_{4}$ HTS, the valence and conduction band edges originate from distinct layers, resulting in a type-II band alignment that promotes efficient electron-hole (e-h) separation. Furthermore, the band alignment can be effectively tuned between type-I and type-II by applying an external electric field and varying the interlayer distance. From the optical absorption spectra of the HTSs, we concluded that the C$_{6}$N$_{6}$/GE and hg-C$_{3}$N$_{4}$/GE exhibit an optical response across a wide frequency range, whereas the C$_{6}$N$_{6}$/hg-C$_{3}$N$_{4}$ HTS shows prominent activity primarily in the ultraviolet region. Using the $G_{0}W_{0}$+BSE approach, the exciton binding energies are also calculated for the gapped systems, namely C$_{6}$N$_{6}$, hg-C$_{3}$N$_{4}$ monolayers, and their HTS (C$_{6}$N$_{6}$/hg-C$_{3}$N$_{4}$), yielding values of 1.01 eV, 1.14 eV, and 1.18 eV, respectively, highlighting strong e-h interactions. Moreover, the band-edge analysis of C$_{6}$N$_{6}$/hg-C$_{3}$N$_{4}$ HTS further favors pronounced interlayer e-h coupling.

CommentsMain Manuscript: 13 figures, 16 pages. Supplemental Material: 9 figures, 6 pages

Journal refPhys. Rev. B 114, 105301 (2026)

DOI:10.1103/1qnh-zvzq

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