Malinský Petr, Slepička Petr, Hnatowicz Vladimír, Svorčík Václav
Department of Solid State Engineering, Institute of Chemical Technology in Prague, Prague, 166 28, Czech Republic.
Nanoscale Res Lett. 2012 May 6;7(1):241. doi: 10.1186/1556-276X-7-241.
Extremely thin gold layers were sputter deposited on glass and silicon substrates, and their thickness and morphology were studied by Rutherford backscattering (RBS) and atomic force microscopy (AFM) methods. The deposited layers change from discontinuous to continuous ones for longer deposition times. While the deposition rate on the silicon substrate is constant, nearly independent on the layer thickness, the rate on the glass substrate increases with increasing layer thickness. The observed dependence can be explained by a simple kinetic model, taking into account different sticking probabilities of gold atoms on a bare glass substrate and regions with gold coverage. Detailed analysis of the shape of the RBS gold signal shows that in the initial stages of the deposition, the gold layers on the glass substrate consist of gold islands with significantly different thicknesses. These findings were confirmed by AFM measurements, too. Gold coverage of the silicon substrate is rather homogeneous, consisting of tiny gold grains, but a pronounced worm-like structure is formed for the layer thickness at electrical continuity threshold. On the glass substrate, the gold clusters of different sizes are clearly observed. For later deposition stages, a clear tendency of the gold atoms to aggregate into larger clusters of approximately the same size is observed. At later deposition stages, gold clusters of up to 100 nm in diameter are formed.
在玻璃和硅基板上溅射沉积极薄的金层,并通过卢瑟福背散射(RBS)和原子力显微镜(AFM)方法研究其厚度和形态。对于更长的沉积时间,沉积层从间断变为连续。虽然硅基板上的沉积速率是恒定的,几乎与层厚度无关,但玻璃基板上的沉积速率随层厚度的增加而增加。所观察到的这种依赖性可以通过一个简单的动力学模型来解释,该模型考虑了金原子在裸露玻璃基板和有金覆盖区域上不同的附着概率。对RBS金信号形状的详细分析表明,在沉积的初始阶段,玻璃基板上的金层由厚度差异显著的金岛组成。这些发现也通过AFM测量得到了证实。硅基板的金覆盖相当均匀,由微小的金颗粒组成,但在电连续性阈值的层厚度下形成了明显的蠕虫状结构。在玻璃基板上,可以清楚地观察到不同尺寸的金簇。在后期沉积阶段,观察到金原子明显倾向于聚集成大致相同尺寸的更大簇。在后期沉积阶段,形成了直径达100纳米的金簇。