利用低温小量子效应计算复杂简并半导体中的300-K迁移率:Ga2O3(会议报告)

D. Look
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引用次数: 0

摘要

通过掺入Fe或Mg, β-Ga2O3具有4.7 eV的高带隙,可以实现半绝缘,从而具有大功率开关所需的高击穿场。令人惊讶的是,通过掺杂Si, β-Ga2O3也可以获得高导电性,这导致了n+的极具潜力的触点和透明电流扩散层。在后一种应用中,目标是实现高电导率(高浓度n和迁移率μ)和可见光和紫外区域的高透明度。最近,我们利用脉冲激光沉积(PLD)在含有1 wt%-SiO2的Ga2O3靶上实现了β-Ga2O3的n = 2 × 1020 cm-3。虽然n与温度无关,但µ不是,通过拟合µvs T,我们可以确定供体ND和受体NA浓度。然而,在较高的温度下,µ受到纵向光学(LO)声子散射的强烈影响,这在Ga2O3(9个LO声子)中比在ZnO, GaN和其他二元半导体(1个LO声子)中要复杂得多。高掺杂的样品还有另一个并发症,即掺杂剂放置的无序性。幸运的是,这种无序导致电导率的小量子修正δ σ,这也受到LO声子的影响。事实上,在低温下σ对T和对磁场B的研究对于理解300 K下的迁移率至关重要。我们演示了在pld生长的β-Ga2O3中ND和NA的计算,假设主要受体是各种电荷态的Ga空位。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Using small low-temperature quantum effects to calculate 300-K mobility in complex degenerate semiconductors: Ga2O3 (Conference Presentation)
With a high bandgap of 4.7 eV, β-Ga2O3 can be made semi-insulating by doping with Fe or Mg and thereby possesses a very high breakdown field necessary for high-powered switches. Somewhat surprisingly, β-Ga2O3 can also be made highly conductive by doping with Si, which leads to great potential for n+ohmic contacts and transparent current spreading layers. In the latter application, the goal is to achieve both high conductivity (high concentration n and mobility μ) and high transparency in the visible and UV regions. Recently we have achieved n = 2 x 1020 cm-3 in β-Ga2O3, using pulsed laser deposition (PLD) with a Ga2O3 target containing 1-wt%-SiO2. Although n is temperature-independent, µ is not, and by fitting µ vs T, we can determine donor ND and acceptor NA concentrations. However, at higher temperatures, µ is strongly affected by longitudinal optical (LO) phonon scattering, which is much more complicated to model in Ga2O3 (9 LO phonons) than in ZnO, GaN, and other binary semiconductors (1 LO phonon). Highly-doped samples have another complication, disorder in the dopant placement. Fortunately, this disorder leads to small quantum corrections delta sigma in the conductivity which are also affected by LO phonons. Indeed, the study of delta sigma vs T and vs magnetic field B at low temperatures is crucial in understanding mobility at 300 K. We demonstrate calculations of ND and NA in PLD-grown β-Ga2O3 under the assumption that the dominant acceptor is the Ga vacancy in various charge states.
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