Krawczyk Mirosław, Pisarek Marcin, Szoszkiewicz Robert, Jablonski Aleksander
Laboratory of Surface Analysis, Institute of Physical Chemistry, Polish Academy of Sciences, Kasprzaka 44/52, 01-224 Warsaw, Poland.
Biological and Chemical Research Centre, Faculty of Chemistry, University of Warsaw, Żwirki Wigury 101, 02-089 Warsaw, Poland.
Materials (Basel). 2020 Aug 14;13(16):3595. doi: 10.3390/ma13163595.
Mo disulfide overlayers with the thickness exceeding 1.77 nm were obtained on Si substrates through mechanical exfoliation. The resulting Mo disulfide flakes were then analyzed ex situ using combination of Auger electron spectroscopy (AES), elastic-peak electron spectroscopy (EPES) and scanning electron microscopy (SEM) in order to characterize their surface chemical composition, electron transport phenomena and surface morphology. Prior to EPES measurements, the Mo disulfide surface was sputter-cleaned and amorphized by 3 kV argon ions, and the resulting S/Mo atomic ratio varied in the range 1.80-1.88, as found from AES measurements. The SEM images revealed single crystalline small-area (up to 15 μm in lateral size) Mo disulfide flakes having polygonal or near-triangular shapes. Such irregular-edged flakes exhibited high crystal quality and thickness uniformity. The inelastic mean free path (IMFP), characterizing electron transport, was evaluated from the relative EPES using Au reference material for electron energies = 0.5-2 keV. Experimental IMFPs, , determined for the AES-measured surface compositions were approximated by the simple function = , where = 0.0289 and = 0.946 were fitted parameters. Additionally, these IMFPs were compared with IMFPs resulting from the two methods: (i) present calculations based on the formalism of the Oswald et al. model; (ii) the predictive equation of Tanuma et al. (TPP-2M) for the measured MoSC surface composition (S/Mo = 1.88), and also for stoichiometric MoS composition. The fitted function was found to be reasonably consistent with the measured, calculated and predicted IMFPs. We concluded that the measured IMFP value at 0.5 keV was only slightly affected by residual carbon contamination at the Mo disulfide surface.
通过机械剥离在硅衬底上获得了厚度超过1.77 nm的二硫化钼覆盖层。然后,使用俄歇电子能谱(AES)、弹性峰电子能谱(EPES)和扫描电子显微镜(SEM)的组合对所得的二硫化钼薄片进行非原位分析,以表征其表面化学成分、电子传输现象和表面形态。在进行EPES测量之前,用3 kV氩离子对二硫化钼表面进行溅射清洗并使其非晶化,从AES测量中发现,所得的S/Mo原子比在1.80 - 1.88范围内变化。SEM图像显示出具有多边形或近三角形形状的单晶小面积(横向尺寸最大为15μm)二硫化钼薄片。这种边缘不规则的薄片表现出高晶体质量和厚度均匀性。使用金参考材料,针对电子能量 = 0.5 - 2 keV,从相对EPES评估表征电子传输的非弹性平均自由程(IMFP)。针对AES测量的表面成分确定的实验IMFP值,通过简单函数 = 进行近似,其中 = 0.0289和 = 0.946是拟合参数。此外,将这些IMFP与两种方法得到的IMFP进行了比较:(i)基于Oswald等人模型形式的当前计算;(ii)针对测量的MoSC表面成分(S/Mo = 1.88)以及化学计量的MoS成分的Tanuma等人的预测方程(TPP - 2M)。发现拟合函数与测量、计算和预测的IMFP合理一致。我们得出结论,在0.5 keV时测量的IMFP值仅受到二硫化钼表面残留碳污染的轻微影响。