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Types of Semiconductors01:20

Types of Semiconductors

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Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
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Predicting Molecular Geometry02:27

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VSEPR Theory for Determination of Electron Pair Geometries
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Fermi Level01:18

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The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
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Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
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When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
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从第一原则中探索原子薄β-TeO的内在和外在类型可变性.

Rafael Costa-Amaral1, Soungmin Bae1, Thi Ngoc Huyen Vu1

  • 1Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan.

ACS applied materials & interfaces
|December 26, 2024
PubMed
概括

内在缺陷不能解释二维β-TeO2.2中的p型导电性. 相反,孔导可能是由杂质状态或基质效应引起的,Bi作为剂显示出希望.

关键词:
两维材料是二维材料.密度-功能理论密度-功能理论兴奋剂的使用 兴奋剂的使用p型导电性的导电性.点缺陷是指点上的缺陷.这就是β-TeO2的含量.

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科学领域:

  • 材料科学 材料科学 材料科学
  • 凝聚物质物理学 凝聚物质物理学
  • 半导体物理 半导体物理

背景情况:

  • 二维 (2D) β-TeO2是一种具有高孔流动性的透明材料,使其对光电子和电源设备具有吸引力.
  • 控制其p型导电性和可配电性的基本机制尚不清楚.
  • 了解这些机制对于优化其在电子应用中的性能至关重要.

研究的目的:

  • 研究内在和外在点缺陷在单层和双层β-TeO2的p型导电性中的作用.
  • 探索在二维β-TeO2.2中实现p型导电性的潜在剂.
  • 为了阐明在这种材料中负责孔导的机制.

主要方法:

  • 在理论计算中使用了Heyd-Scuseria-Ernzerhof (HSE) + D3混合函数.
  • 研究了单层和双层β-TeO2的内在和外在点缺陷.
  • 研究了使用十种三价元素的替代性兴奋剂.

主要成果:

  • 大多数内在缺陷不会导致2Dβ-TeO2.2中的p型兴奋剂.
  • 和污染可以降低p型导电性.
  • 孔导电很可能是由于通过局部杂质状态或基质效应跳跃而引起的.
  • (Bi) 显示了浅层的受体水平,但所有兴奋剂都会产生深层的局部状态.
  • 单层β-TeO2由于减少自我补偿,比双层具有优势.

结论:

  • 内在缺陷不是2Dβ-TeO2.2中p型导电性的主要来源.
  • 提出了诸如跳跃导电和基板效应等替代机制.
  • 石兴奋剂是一种潜在的途径,但缺陷状态需要仔细管理.
  • 单层2Dβ-TeO2由于减少自我补偿,对p型兴奋剂具有前景,为电子设备的缺陷工程提供了一条途径.