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相关概念视频

Ionic Crystal Structures02:42

Ionic Crystal Structures

18.1K
Ionic crystals consist of two or more different kinds of ions that usually have different sizes. The packing of these ions into a crystal structure is more complex than the packing of metal atoms that are the same size.
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
18.1K
Semiconductors01:22

Semiconductors

1.9K
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
1.9K
Types of Semiconductors01:20

Types of Semiconductors

1.8K
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...
1.8K
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

1.4K
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
1.4K
MOS Capacitor01:25

MOS Capacitor

1.8K
A Metal-Oxide-Semiconductor (MOS) capacitor is a fundamental structure used extensively in semiconductor device technology, particularly in the fabrication of integrated circuits and MOSFETs (metal-oxide-semiconductor field-effect transistors). The MOS capacitor consists of three layers: a metal gate, a dielectric oxide, and a semiconductor substrate.
The metal gate is typically made from highly conductive materials such as aluminum or polysilicon. Beneath the metal gate lies a thin layer of...
1.8K
Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

147
Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...
147

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Atmospheric Pressure Fabrication of Large-Sized Single-Layer Rectangular SnSe Flakes
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基于[SnSe4](4-) 离子的中介结构半导体中多种多孔组织.

P N Trikalitis1, K K Rangan, T Bakas

  • 1Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA.

Nature
|April 5, 2001
PubMed
概括
此摘要是机器生成的。

研究人员使用一种新的超分子组装方法开发了新的中孔金属化半导体. 这些材料具有可调节的带隙和有序的孔状结构,可用于光电子和光催化.

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科学领域:

  • 材料科学 材料科学 材料科学
  • 固态化学 固态化学
  • 纳米技术纳米技术

背景情况:

  • 具有纳米和中等尺度孔的半孔性材料对于光电子和量子束物理学的应用至关重要.
  • 在半孔方面取得了重大进展,但非氧化类型的类似物仍然难以合成.

研究的目的:

  • 开发一种合成策略,用于制造一种新的类型的中孔金属素固体.
  • 探索这些新型材料的结构和电子特性.

主要方法:

  • 四面体Zintl离子[SnSe4]4-与过渡金属 (Mn,Fe,Co,Zn,Cd,Hg) 的超分子组合.
  • 使用 cetylpyridinium (CP) 表面活性分子来直接形成 mesostructure.
  • 由此产生的材料的表征用一般公式 (CP)4-2xMxSnSe4.4.

主要成果:

  • 成功合成了具有均孔径 (35-40 Å) 的半导体化物质.
  • 观察到各种各样的孔隙安排,包括无序的虫洞,六角和立方相,取决于合成条件和使用的金属.
  • 所有合成的化合物都表现出中等带隙半导体特性,范围从1.4到2.5 eV.

结论:

  • 一种新的合成策略使得各种中孔金属化物的制备成为可能.
  • 这些材料具有可调节的电子特性和有序的多孔结构.
  • 预计这些半导体多孔网络在光电子,光合作用和光催化领域有潜在的应用.