首页> 外文学位 >ELECTRON FIELD EMISSION TUNNELING SPECTROSCOPY OF PLATINUM GROUP AND TUNGSTEN METALS IN THE PRESENCE OF MOLECULAR GAS AND NOBLE METAL ADSORBATES.
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ELECTRON FIELD EMISSION TUNNELING SPECTROSCOPY OF PLATINUM GROUP AND TUNGSTEN METALS IN THE PRESENCE OF MOLECULAR GAS AND NOBLE METAL ADSORBATES.

机译:分子气体和贵金属吸附剂存在下铂族和钨金属的电子发射隧穿光谱

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摘要

Using field-electron energy-distribution, (FEED), measurements, three adsorbate/substrate systems have been investigated. Molecular gases, (hydrogen, carbon monoxide, oxygen, nitrogen, nitric oxide, ammonia and hydrazine), have been adsorbed on several crystal faces of iridium. Gold and copper have been adsorbed on iridium, rhodium and platinum. Finally gold and copper have been adsorbed on crystal faces of tungsten.; In results similar but not identical to those of other experimentalists, we find that on W{lcub}100{rcub} the surface state present in the clean FEED spectrum disappears immediately as adsorption of gold and copper begins. However, at both one and two monolayer coverages, the surface state and, in fact, the entire clean energy spectrum returns. We believe these results can be explained in terms of theoretical models and the symmetry of the surface atomic layer. The symmetry is broken by the initial adsorbate coverage but is reestablished at integral monolayer coverages by perfect pseudomorphic ordering of the overlayers.; For copper the results depend on substrate temperature. After four monolayers of copper on a 530K substrate an extremely large resonance feature appears at 0.8 eV. This is probably caused by reconstruction of copper into its normal face-centered-cubic structure and may then be a manifestation of the surface state which is seen on Cu{lcub}111{rcub}. Copper deposited on colder substrates behaves like gold except for minor enhancement at 0.8 eV.; Copper on the W{lcub}111{rcub} plane produces results related but not identical to those on W{lcub}100{rcub}. At high temperatures and coverages a very large peak is again seen although it shows a large energy shift with coverage. When copper is deposited at 78K the clean spectrum remains for a significant fraction of a monolayer. This is interpreted as due to nucleated 1 x 1 island growth of the adsorbed layer such that the surface symmetry is not destroyed.; Interpretation of the results for copper and gold on the platinum group metals is inhibited by the lack of experimental or theoretical work with which to compare the present results. A large binding energy anisotropy between the Ir{lcub}111{rcub} plane and the emitter surface around it is found for both gold and copper. Either metal rapidly diffuses off the flat {lcub}111{rcub} plane at 600K. However, after a monolayer has accumulated on the surrounding areas, invasion of the {lcub}111{rcub} plane begins. A number of work-function and emission micrograph phenomena are found to be associated with this effect.; The most common result obtained in the gas adsorption experiments is that the interesting d-band energy structure found on the clean iridium surface is removed, leaving a free-electron-like FEED spectrum. In several instances this result is preceded by interesting enhancement or suppression of certain regions of the spectra. Unfortunately without a quantitative theory of field emission in the presence of adsorbates we are usually unable to interpret such results.; Complex phenomena are observed for nitric oxide. On Ir{lcub}111{rcub} adsorption is associative and thermal desorption occurs between 400K and 530K. On Ir{lcub}100{rcub} NO is probably molecular from 78K to 400K but dissociates before desorption at around 600K. The work-functions and energy spectra appear to be dominated by nitrogen since similar results are obtained with nitrogen, ammonia and hydrazine. It is not clear what happens to the oxygen which other experiments have shown not to desorb until 800 to 1270K. Experiments with nitric oxide on a macroscopic Ir{lcub}100{rcub} crystal should be performed.
机译:使用场电子能量分布(FEED)进行测量,研究了三种吸附物/基质系统。分子气体(氢气,一氧化碳,氧气,氮气,一氧化氮,氨和肼)已被吸附在铱的多个晶面上。金和铜已被吸附在铱,铑和铂上。最后,金和铜已被吸附在钨的晶体表面上。在与其他实验者相似但不相同的结果中,我们发现在W {lcub} 100 {rcub}上,随着金和铜的吸附开始,干净的FEED光谱中存在的表面态立即消失。但是,在一个和两个单层覆盖率下,表面状态以及实际上整个清洁能谱都将返回。我们相信这些结果可以用理论模型和表面原子层的对称性来解释。对称性被最初的吸附物覆盖率破坏,但通过叠加器的完美伪态排序在整体单层覆盖率中得以重新建立。对于铜,结果取决于基板温度。在530K基板上形成四个单层铜之后,在0.8 eV处会出现极大的共振特征。这可能是由于将铜重新构造成其正常的面心立方结构所致,然后可能是在Cu {lcub} 111 {rcub}上看到的表面状态的体现。沉积在较冷基板上的铜的行为类似于金,只是在0.8 eV处有较小的增强。 W {lcub} 111 {rcub}平面上的铜产生的结果与W {lcub} 100 {rcub}上的结果相关但不相同。在高温和高覆盖率下,尽管它显示出覆盖范围内的巨大能量漂移,但仍会看到一个非常大的峰。当铜以78K沉积时,干净的光谱保留了很大一部分单层。可以认为这是由于吸附层有核的1×1岛状生长,因此表面对称性没有破坏。缺乏用于比较当前结果的实验​​或理论工作,无法解释铂族金属上的铜和金的结果。对于金和铜,都发现Ir {lcub} 111 {rcub}平面与其周围的发射极表面之间存在很大的结合能各向异性。两种金属都以600K的速度从平坦的{lcub} 111 {rcub}平面迅速扩散。但是,在单分子层已在周围区域积聚之后,{lcub} 111 {rcub}平面开始入侵。已发现许多功函数和发射显微照片现象与这种效应有关。在气体吸附实验中获得的最常见结果是,去除了在干净的铱表面上发现的有趣的d带能量结构,从而留下了类似自由电子的FEED光谱。在某些情况下,此结果之前是对光谱某些区域的有趣增强或抑制。不幸的是,如果没有在吸附剂存在下的场发射定量理论,我们通常无法解释这种结果。一氧化氮观察到复杂的现象。在Ir {lcub} 111 {rcub}上,吸附是缔合的,热解吸发生在400K和530K之间。在Ir {lcub} 100 {rcub}上,NO可能是78K至400K的分子,但在600K左右解吸之前会解离。功函数和能谱似乎由氮决定,因为用氮,氨和肼获得了相似的结果。目前尚不清楚其他实验显示直到800至1270K才解吸的氧气发生了什么变化。应该在宏观Ir {lcub} 100 {rcub}晶体上使用一氧化氮进行实验。

著录项

  • 作者单位

    Cornell University.;

  • 授予单位 Cornell University.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 1981
  • 页码 182 p.
  • 总页数 182
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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