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Microcalorimetric measurements of the heat of absorption of Pb on well-defined oxides: MgO(100) and p(2*1)-oxide on Mo(100)

机译:微量热法测量铅在明确定义的氧化物上的吸收热:Mg​​O(100)和Mo(100)上的p(2 * 1)-氧化物

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The energetics of Pb film grown at 300 K on two well-defined oxides [a MgO(100) thin film and a p(2xl)-oxide on Mo(100)] have been measured using single-crystal absorption microcalorimetry. The evolution of the film morphology was followed using Auger electron spectroscopy (AES). An initial heat of absorption of 103 kJ/mol is observed for the Pb/MgO(100) system. Auger results indicate that this is due to the formation of an -20 atom Pb island in the first pulse of Pb gas incident on the MgO(lOO) surface. This allows the extraction bf a Pb-MgO(loo) bond energy of -32::!:2 kJ/mol in the small two-dimensional particles formed ift the first pulse. As more Pb is deposited onto the MgO(loo) surface, the Pb forms three-dimensionalcislands. The integral of the heats of absorption up to high coverage indicates an adhesion energy of76.5::!:-20.uJ/cm2 for large 3D Pb particles to the MgO(100) substrate. This indicates a Pb-MgO(loo) bond energy of 49::!: 13 kJ/rnol at the 3D interface. Similar analyses of the Pb/p(2X 1)-oxide on Mo(100) surface give an initial heat of absorption of 146.2 kJ/mol and an adhesion energy of 82.5::!:20 .uJ/cm2 for thick Pb films. This indicates a bond energy of 52::!: 12 kJ/mol for a Pb atom to this surface at the interface of a thick Pb film. The metal's sticking probabilities as a function of coverage and the coverage-dependent changes in optical reflectivity were measured. For the Pb/MgO(100) system, an initial sticking probability of 0.70 at 300 K was observed, whereas for the Pb/p(2x 1)-oxide on Mo(100) surface unit sticking probability was observed. The relationship between these quantities and the adsorption energetics is discussed.
机译:已经使用单晶吸收量热法测量了在两种定义明确的氧化物上以300 K生长的Pb薄膜的能量[MgO(100)薄膜和Mo(100)上的p(2xl)-氧化物]。使用俄歇电子能谱(AES)跟踪薄膜形态的演变。对于Pb / MgO(100)系统,观察到初始吸收热为103 kJ / mol。俄歇结果表明,这是由于在入射到MgO(100)表面的Pb气体的第一个脉冲中形成了-20原子的Pb岛。这允许提取形成于第一脉冲之后的二维小颗粒中-32 ::!:2 kJ / mol的Pb-MgO(loo)键能。随着更多的Pb沉积到MgO(loo)表面上,Pb形成了三维顺式晶界。吸收热的积分直到高覆盖率才表明,大3D Pb粒子与MgO(100)衬底的粘附能为76.5 ::!:-20.uJ / cm2。这表明在3D界面上Pb-MgO(loo)键能为49 ::!:13 kJ / rnol。 Mo(100)表面上的Pb / p(2X 1)-氧化物的类似分析得出厚Pb膜的初始吸收热为146.2 kJ / mol,粘附能为82.5 ::!:20 uJ / cm2。这表明在厚的Pb膜的界面上,一个Pb原子到该表面的结合能为52 ::!:12 kJ / mol。测量了金属的粘附概率与覆盖率的关系以及取决于覆盖率的光反射率变化。对于Pb / MgO(100)系统,在300 K时观察到初始黏附概率为0.70,而对于Mo(100)表面单元上的Pb / p(2x 1)-氧化物,则观察到黏附概率。讨论了这些量与吸附能之间的关系。

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