Department of Chemistry and Biochemistry, University of Colorado, Boulder, Colorado 80309-0215, USA.
J Chem Phys. 2017 Feb 7;146(5):052819. doi: 10.1063/1.4973310.
The thermal atomic layer etching (ALE) of AlO can be performed using sequential and self-limiting reactions with trimethylaluminum (TMA) and hydrogen fluoride (HF) as the reactants. The atomic layer deposition (ALD) of AlF can also be accomplished using the same reactants. This paper examined the competition between AlO ALE and AlF ALD using in situ Fourier transform infrared (FTIR) vibrational spectroscopy measurements on AlO ALD-coated SiO nanoparticles. The FTIR spectra could observe an absorbance loss of the Al-O stretching vibrations during AlO ALE or an absorbance gain of the Al-F stretching vibrations during AlF ALD. The transition from AlF ALD to AlO ALE occurred versus reaction temperature and was also influenced by the N or He background gas pressure. Higher temperatures and lower background gas pressures led to AlO ALE. Lower temperatures and higher background gas pressures led to AlF ALD. The FTIR measurements also monitored AlCH* and HF species on the surface after the TMA and HF reactant exposures. The loss of AlCH* and HF species at higher temperatures is believed to play a vital role in the transition between AlF ALD at lower temperatures and AlO ALE at higher temperatures. The change between AlF ALD and AlO ALE was defined by the transition temperature. Higher transition temperatures were observed using larger N or He background gas pressures. This correlation was associated with variations in the N or He gas thermal conductivity versus pressure. The fluorination reaction during AlO ALE is very exothermic and leads to temperature rises in the SiO nanoparticles. These temperature transients influence the AlO etching. The higher N and He gas thermal conductivities are able to cool the SiO nanoparticles more efficiently and minimize the size of the temperature rises. The competition between AlO ALE and AlF ALD using TMA and HF illustrates the interplay between etching and growth and the importance of substrate temperature. Background gas pressure also plays a key role in determining the transition temperature for nanoparticle substrates.
使用三甲基铝(TMA)和氢氟酸(HF)作为反应物,可以进行热原子层刻蚀(ALE)以去除 AlO。也可以使用相同的反应物来实现 AlF 的原子层沉积(ALD)。本文通过原位傅里叶变换红外(FTIR)振动光谱测量,研究了 AlO ALE 和 AlF ALD 之间的竞争,这些测量是在 AlO ALD 涂覆的 SiO 纳米颗粒上进行的。FTIR 光谱可以观察到 Al-O 伸缩振动在 AlO ALE 过程中的吸收损失,或 Al-F 伸缩振动在 AlF ALD 过程中的吸收增加。在反应温度下,AlF ALD 到 AlO ALE 的转变会发生,并且还会受到 N 或 He 背景气体压力的影响。较高的温度和较低的背景气体压力会导致 AlO ALE。较低的温度和较高的背景气体压力会导致 AlF ALD。FTIR 测量还在 TMA 和 HF 反应物暴露后监测表面上的 AlCH和 HF 物种。在较高温度下,AlCH和 HF 物种的损失被认为在低温下的 AlF ALD 和高温下的 AlO ALE 之间的转变中起着至关重要的作用。AlF ALD 和 AlO ALE 之间的变化由转变温度定义。较高的转变温度在使用较大的 N 或 He 背景气体压力时观察到。这种相关性与 N 或 He 气体导热率随压力的变化有关。AlO ALE 期间的氟化反应非常放热,导致 SiO 纳米颗粒的温度升高。这些温度瞬变会影响 AlO 的刻蚀。较高的 N 和 He 气体导热率能够更有效地冷却 SiO 纳米颗粒,并最小化温度升高的幅度。使用 TMA 和 HF 的 AlO ALE 和 AlF ALD 之间的竞争说明了刻蚀和生长之间的相互作用,以及衬底温度的重要性。背景气体压力在确定纳米颗粒衬底的转变温度方面也起着关键作用。