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Simulated measurement of small metal clusters by frequency-modulation non-contact atomic force microscopy

机译:调频非接触原子力显微镜对小型金属团簇的模拟测量

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The apparent height and lateral extent of very small metallic clusters and particles adsorbed on flat substrates have been calculated for frequency-modulation non-contact atomic force microscopy (ncAFM). The ncAFM scanning tip was modelled as a Si sphere covered by 1 nm of SiO_2. This tip sphere of either 5 or 20 nm total radius (including an SiO_2 layer) is attached to a cantilever of spring constant k = 40Nm~(-1) and oscillated with a 10 nm amplitude. The tip was rastered across the centre of a single cluster of Pd atoms or a single Pd particle located on a flat continuum substrate of alumina or Pd. The clusters were one-atom-thick close-packed arrangements of 19 or 91 atoms (1.4 or 3.0 nm wide); the particles were continuum spheres of diameter 2.0 or 4.0 nm. The tip - substrate and tip-particle interactions were modelled with 6 - 12 Lennard-Jones potentials. The attractive interaction was taken to be the London - van der Waals dispersion interaction whose magnitude was estimated from Hamaker constants calculated from bulk optical constants of Si, SiO_2, Pd, and alumina. The repulsive interaction was determined from estimates of the atomic radii using densities of the bulk materials. These simulations show that the apparent heights of particles imaged by ncAFM range from just 12 percent of the actual height for the smallest Pd cluster on a Pd substrate to 95percent of the actual height for the largest Pd particle on an alumina substrate. The apparent widths of the clusters were similar to those in contact AFM. These results show the most accurate height measurements occur when the lateral extent of the cluster or particle is comparable to or larger than the radius of the tip and when the Hamaker constant for the interaction of the tip with a cluster or particle is larger than that for the tip with the substrate.
机译:对于频率调制非接触原子力显微镜(ncAFM),已经计算出了非常小的金属簇和吸附在平坦基底上的颗粒的表观高度和横向范围。将ncAFM扫描尖端建模为被1 nm SiO_2覆盖的Si球。这个总半径为5或20 nm的尖端球体(包括SiO_2层)连接到弹簧常数k = 40Nm〜(-1)的悬臂上,并以10 nm的振幅振荡。尖端跨单个的Pd原子簇或位于氧化铝或Pd的连续连续基底上的单个Pd颗粒的中心栅格化。这些簇是19或91个原子(宽1.4或3.0 nm宽)的单原子厚紧密堆积排列;颗粒是直径为2.0或4.0 nm的连续球。尖端-底物和尖端-颗粒的相互作用是用6-12 Lennard-Jones势建模的。有吸引力的相互作用被认为是伦敦-范德华分散相互作用,其大小是根据由Si,SiO_2,Pd和氧化铝的体光学常数计算出的Hamaker常数估算的。排斥相互作用是通过使用散装材料的密度从原子半径的估计值确定的。这些模拟表明,ncAFM成像的粒子的表观高度范围仅为Pd基板上最小Pd簇的实际高度的12%到氧化铝基板上最大Pd颗粒的实际高度的95%。簇的表观宽度类似于接触式原子力显微镜。这些结果表明,当团簇或颗粒的横向范围等于或大于尖端的半径,并且当尖端与团簇或颗粒的相互作用的Hamaker常数大于或大于尖端的半径时,会发生最准确的高度测量。尖端与基材。

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