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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Understanding Thermal Evolution and Monolayer Doping of Sulfur-Passivated GaAs(100)
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Understanding Thermal Evolution and Monolayer Doping of Sulfur-Passivated GaAs(100)

机译:了解硫钝化GaAs(100)的热进化和单层掺杂

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Monolayer doping (MLD) is an attractive method to precisely tailor dopant profiles for nanoelectronic semiconductor devices. The approach has been demonstrated for a number of different dopant/substrate combinations, but the mechanistic understanding of reactions of dopant-containing monolayers, intermediate structures, and the role of capping layers has suffered from lack of in situ characterization. Here, we investigate the thermal evolution of sulfur-passivated GaAs(100) without any additional capping layers in the context of MLD, using a combination of in situ X-ray photoemission spectroscopy (XPS), low-energy ion scattering (LEIS), and infrared (IR) absorption spectroscopy. In the case of (NH4)(2)S-passivated GaAs(100), the intermediate structure that precedes subsurface diffusion is characterized by a (2 X 1) reconstruction that has previously been ascribed to several different dimer moieties. These dimer structures are currently unresolved yet could influence subsequent doping processes. By use of LEIS, temperature-dependent measurements provide unambiguous information on the chemical origin of the intermediate (2 x 1) reconstruction, originating from the dimerization of S atoms. Annealing beyond 813 K results in a loss of the surface S signal and is accompanied by free-carrier absorption in IR spectra, consistent with doping. The magnitude of this absorption and the carrier densities extracted from these data indicate that peak doping levels exceeding 10(20) cm(-3) can be achieved and that the free carrier concentration within a shallow profile can be tuned by adjusting the annealing time.
机译:单层掺杂(MLD)是一种有吸引力的方法,可以精确地定制纳米电子半导体器件的掺杂剂型材。该方法已经证明了许多不同的掺杂剂/衬底组合,而是对含掺杂剂的单层,中间结构和封端层的作用的机制理解缺乏原位表征。在这里,我们研究了在MLD的上下文中没有任何额外的覆盖层的硫钝化的GaAs(100)的热量演变,使用原位X射线照相激光谱(XPS),低能量离子散射(唯一),和红外(IR)吸收光谱。在(NH4)(2)S钝化的GaAs(100)的情况下,前表面扩散的中间结构的特征在于(2×1)重建,其先前已归因于几个不同的二聚体部分。这些二聚体结构目前尚未解决,但可能影响随后的掺杂过程。通过使用光,温度依赖的测量提供了关于中间体(2×1)重建的化学来源的明确信息,来自S原子的二聚体。退火超过813K导致表面信号的损失,并伴随着IR光谱的自由载体吸收,与掺杂一致。从这些数据提取的这种吸收和载体密度的幅度表明可以实现超过10(20 )cm(-3)的峰值掺杂水平,并且可以通过调节退火时间来调谐浅轮廓内的自由载流子浓度。

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