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Field enhancement factors and self-focus functions manifesting in field emission resonances in scanning tunneling microscopy

机译:扫描隧道显微镜在场发射共振中表现出的场增强因子和自聚焦功能

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Field emission (FE) resonance (or Gundlach oscillation) in scanning tunneling microscopy (STM) is a phenomenon in which the FE electrons emitted from the microscope tip couple into the quantized standing-wave states within the STM tunneling gap. Although the occurrence of FE resonance peaks can be semi-quantitatively described using the triangular potential well model, it cannot explain the experimental observation that the number of resonance peaks may change under the same emission current. This study demonstrates that the aforementioned variation can be adequately explained by introducing a field enhancement factor that is related to the local electric field at the tip apex. The peak number of FE resonances increases with the field enhancement factor. The peak intensity of the FE resonance on the reconstructed Au(111) surface varies in the face-center cubic, hexagonal-close-packed, and ridge regions, thus providing the contrast in the mapping through FE resonances. The mapping contrast is demonstrated to be nearly independent of the tip-sample distance, implying that the FE electron beam is not divergent because of a self-focus function intrinsically involved in the STM configuration.
机译:扫描隧道显微镜(STM)中的场发射(FE)共振(或Gundlach振荡)是一种现象,其中从显微镜尖端发射的FE电子耦合到STM隧道间隙内的量化驻波状态。尽管可以使用三角势阱模型对FE共振峰的出现进行半定量描述,但它不能解释在相同发射电流下共振峰数目可能发生变化的实验观察。这项研究表明,通过引入与尖端顶部局部电场相关的场增强因子,可以充分解释上述变化。 FE共振的峰值数量随场增强因子而增加。重构的Au(111)表面上的FE共振的峰值强度在面心立方,六方密堆积和脊区域中变化,因此在通过FE共振进行映射时提供了对比度。映射对比度被证明几乎与尖端样品距离无关,这意味着FE电子束不会发散,因为STM配置固有地具有自聚焦功能。

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