Research group PLASMANT, Department of Chemistry,, University of Antwerp , Universiteitsplein 1, 2610 Antwerp, Belgium.
Acc Chem Res. 2017 Apr 18;50(4):796-804. doi: 10.1021/acs.accounts.6b00564. Epub 2017 Mar 1.
The continuous miniaturization of nanodevices, such as transistors, solar cells, and optical fibers, requires the controlled synthesis of (ultra)thin gate oxides (<10 nm), including Si gate-oxide (SiO) with high quality at the atomic scale. Traditional thermal growth of SiO on planar Si surfaces, however, does not allow one to obtain such ultrathin oxide due to either the high oxygen diffusivity at high temperature or the very low sticking ability of incident oxygen at low temperature. Two recent techniques, both operative at low (room) temperature, have been put forward to overcome these obstacles: (i) hyperthermal oxidation of planar Si surfaces and (ii) thermal or plasma-assisted oxidation of nonplanar Si surfaces, including Si nanowires (SiNWs). These nano-oxidation processes are, however, often difficult to study experimentally, due to the key intermediate processes taking place on the nanosecond time scale. In this Account, these Si nano-oxidation techniques are discussed from a computational point of view and compared to both hyperthermal and thermal oxidation experiments, as well as to well-known models of thermal oxidation, including the Deal-Grove, Cabrera-Mott, and Kao models and several alternative mechanisms. In our studies, we use reactive molecular dynamics (MD) and hybrid MD/Monte Carlo simulation techniques, applying the Reax force field. The incident energy of oxygen species is chosen in the range of 1-5 eV in hyperthermal oxidation of planar Si surfaces in order to prevent energy-induced damage. It turns out that hyperthermal growth allows for two growth modes, where the ultrathin oxide thickness depends on either (1) only the kinetic energy of the incident oxygen species at a growth temperature below T = 600 K, or (2) both the incident energy and the growth temperature at a growth temperature above T. These modes are specific to such ultrathin oxides, and are not observed in traditional thermal oxidation, nor theoretically considered by already existing models. In the case of thermal or plasma-assisted oxidation of small Si nanowires, on the other hand, the thickness of the ultrathin oxide is a function of the growth temperature and the nanowire diameter. Below T, which varies with the nanowire diameter, partially oxidized SiNW are formed, whereas complete oxidation to a SiO nanowire occurs only above T. In both nano-oxidation processes at lower temperature (T < T), final sandwich c-Si|SiO|a-SiO structures are obtained due to a competition between overcoming the energy barrier to penetrate into Si subsurface layers and the compressive stress (∼2-3 GPa) at the Si crystal/oxide interface. The overall atomic-simulation results strongly indicate that the thickness of the intermediate SiO (x < 2) region is very limited (∼0.5 nm) and constant irrespective of oxidation parameters. Thus, control over the ultrathin SiO thickness with good quality is indeed possible by accurately tuning the oxidant energy, oxidation temperature and surface curvature. In general, we discuss and put in perspective these two oxidation mechanisms for obtaining controllable ultrathin gate-oxide films, offering a new route toward the fabrication of nanodevices via selective nano-oxidation.
纳米器件(如晶体管、太阳能电池和光纤)的不断小型化需要控制合成(超)薄栅极氧化物(<10nm),包括在原子尺度上具有高质量的 Si 栅极氧化物(SiO)。然而,传统的在平面 Si 表面上热生长 SiO 由于高温下氧的高扩散率或低温下入射氧的极低附着能力,无法获得如此超薄的氧化物。最近提出了两种在低温(室温)下操作的技术来克服这些障碍:(i)平面 Si 表面的超热氧化和(ii)非平面 Si 表面的热或等离子体辅助氧化,包括 Si 纳米线(SiNWs)。然而,由于发生在纳秒时间尺度上的关键中间过程,这些纳米氧化过程通常很难进行实验研究。在本说明中,从计算的角度讨论了这些 Si 纳米氧化技术,并将其与超热和热氧化实验以及众所周知的热氧化模型(包括 Deal-Grove、Cabrera-Mott 和 Kao 模型以及几种替代机制)进行了比较。在我们的研究中,我们使用反应分子动力学(MD)和混合 MD/Monte Carlo 模拟技术,应用 Reax 力场。在平面 Si 表面的超热氧化中,选择氧种的入射能在 1-5 eV 的范围内,以防止能量诱导的损伤。事实证明,超热生长允许两种生长模式,其中超薄氧化物的厚度取决于(1)仅在低于 T = 600 K 的生长温度下入射氧种的动能,或(2)在高于 T 的生长温度下入射能和生长温度。这些模式是这种超薄氧化物特有的,在传统的热氧化中观察不到,也没有已有的模型理论考虑到。另一方面,在小 Si 纳米线的热或等离子体辅助氧化的情况下,超薄氧化物的厚度是生长温度和纳米线直径的函数。在低于 T 的温度下(随纳米线直径而变化),形成部分氧化的 SiNW,而只有在高于 T 时才会发生完整氧化成 SiO 纳米线。在较低温度(T < T)下的两种纳米氧化过程中,由于穿透 Si 次表面层的能量势垒和 Si 晶体/氧化物界面处的压缩应力(2-3 GPa)之间的竞争,最终获得了 c-Si|SiO|a-SiO 的三明治结构。整体原子模拟结果强烈表明,中间 SiO(x < 2)区域的厚度非常有限(0.5nm)且保持不变,与氧化参数无关。因此,通过精确调整氧化剂能量、氧化温度和表面曲率,可以确实控制具有良好质量的超薄 SiO 厚度。总的来说,我们讨论并从这两种获得可控超薄栅极氧化物薄膜的氧化机制的角度出发,为通过选择性纳米氧化制造纳米器件提供了新途径。