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Atomic Structure01:33

Atomic Structure

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Overview
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Atomic Mass01:52

Atomic Mass

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Atoms — and the protons, neutrons, and electrons that compose them — are extremely small. For example, a carbon atom weighs less than 2 × 10−23 g. When describing the properties of tiny objects such as atoms, we use appropriately small units of measure, such as the atomic mass unit (amu). The amu was originally defined based on hydrogen, the lightest element, then later in terms of oxygen. Since 1961, it has been defined with regard to the most abundant isotope of carbon, atoms of which...
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Atomic Orbitals02:44

Atomic Orbitals

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An atomic orbital represents the three-dimensional regions in an atom where an electron has the highest probability to reside. The radial distribution function indicates the total probability of finding an electron within the thin shell at a distance r from the nucleus. The atomic orbitals have distinct shapes which are determined by l, the angular momentum quantum number. The orbitals are often drawn with a boundary surface, enclosing densest regions of the cloud.
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The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
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Hybridization of Atomic Orbitals I03:24

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The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
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The Energies of Atomic Orbitals03:21

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In an atom, the negatively charged electrons are attracted to the positively charged nucleus. In a multielectron atom, electron-electron repulsions are also observed. The attractive and repulsive forces are dependent on the distance between the particles, as well as the sign and magnitude of the charges on the individual particles. When the charges on the particles are opposite, they attract each other. If both particles have the same charge, they repel each other.
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Quantitative Atomic-Site Analysis of Functional Dopants/Point Defects in Crystalline Materials by Electron-Channeling-Enhanced Microanalysis
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对二维材料和设备的非破坏性原子缺陷量化.

Yucheng Yang1, Kaikui Xu1, Tara Peña2

  • 1Department of Aerospace and Mechanical Engineering, University of Notre Dame, Notre Dame, Indiana 46556, United States.

ACS applied materials & interfaces
|February 6, 2026
PubMed
概括

侧向力显微镜 (LFM) 提供了一种快速,非破坏性的方法,用于绘制WSe2和WS2等二维半导体中的原子缺陷. 这种技术超过了拉曼光谱的灵敏度,有助于材料生长和设备制造分析.

关键词:
两维材料是二维材料.拉曼光谱法 拉曼光谱法 拉曼光谱法原子力显微镜的原子力显微镜.缺陷 缺陷 缺陷 缺陷 缺陷设备设备的设备设备的设备.过渡金属二甲基二甲基化物

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科学领域:

  • 材料科学 材料科学 材料科学
  • 纳米技术纳米技术
  • 表面科学是一门学科.

背景情况:

  • 描述二维半导体中的原子缺陷对于优化增长和设备性能至关重要.
  • 目前的缺陷计量方法通常是缓慢的,破坏性的,或缺乏足够的灵敏度.

研究的目的:

  • 引入和验证横向力显微镜 (LFM) 作为2D材料中原子缺陷表征的非破坏性技术.
  • 评估LFM在各种2D材料,基板和设备结构中的灵敏度和适用性.

主要方法:

  • 使用横向力显微镜 (LFM) 绘制单层二化 (WSe2) 和二硫化 (WS2) 的表面缺陷.
  • 应用于二氧化 (SiO2) 和蓝宝石基板上的材料以及WSe2晶体管中的LFM.
  • 将LFM缺陷检测极限与传统拉曼光谱法进行比较.

主要成果:

  • 在不同基板和晶体管上,LFM成功地绘制了WSe2和WS2的表面缺陷.
  • 该技术检测出缺陷密度明显低于拉曼光谱法可测量的缺陷密度.
  • 与成长膜相比,LFM显示WSe2晶体管的缺陷密度更高,表明制造引起的缺陷.
  • 证明了LFM在悬浮和聚合物支持的2D材料中检测缺陷的能力.

结论:

  • 侧向力显微镜 (LFM) 是一种高度敏感的,非破坏性的方法,用于2D半导体中的原子缺陷特征.
  • LFM为监控二维材料生长和识别设备制造过程中引入的缺陷提供了宝贵的见解.
  • 这种技术扩大了缺陷计量学的范围,用于先进的二维材料应用.