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相关概念视频

Structures of Solids02:22

Structures of Solids

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Solids in which the atoms, ions, or molecules are arranged in a definite repeating pattern are known as crystalline solids. Metals and ionic compounds typically form ordered, crystalline solids. A crystalline solid has a precise melting temperature because each atom or molecule of the same type is held in place with the same forces or energy. Amorphous solids or non-crystalline solids (or, sometimes, glasses) which lack an ordered internal structure and are randomly arranged. Substances that...
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Network Covalent Solids02:18

Network Covalent Solids

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Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
16.2K
Molecular and Ionic Solids02:54

Molecular and Ionic Solids

20.0K
Crystalline solids are divided into four types: molecular, ionic, metallic, and covalent network based on the type of constituent units and their interparticle interactions.
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
20.0K
Metallic Solids02:37

Metallic Solids

20.6K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
20.6K
Molecular Comparison of Gases, Liquids, and Solids02:26

Molecular Comparison of Gases, Liquids, and Solids

54.9K
Particles in a solid are tightly packed together (fixed shape) and often arranged in a regular pattern; in a liquid, they are close together with no regular arrangement (no fixed shape); in a gas, they are far apart with no regular arrangement (no fixed shape). Particles in a solid vibrate about fixed positions (cannot flow) and do not generally move in relation to one another; in a liquid, they move past each other (can flow) but remain in essentially constant contact; in a gas, they move...
54.9K
Energy Bands in Solids01:01

Energy Bands in Solids

2.0K
Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
 Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
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毫米级单晶半导体MoTe2通过固态相变

Xiaolong Xu1,2, Shulin Chen3, Shuai Liu1

  • 1State Key Lab for Artificial Microstructure & Mesoscopic Physics, School of Physics , Peking University , Beijing 100871 , China.

Journal of the American Chemical Society
|January 12, 2019
PubMed
概括
此摘要是机器生成的。

研究人员使用受控固态相转换将多晶二化物 (MoTe2) 转化为单晶2H-MoTe2. 这一突破使得晶圆尺度的二维半导体和先进电子的新型异构结构成为可能.

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科学领域:

  • 材料科学
  • 凝聚物质物理学
  • 纳米技术

背景情况:

  • 二化物 (MoTe2) 具有独特的特性,因为它有两个不同的阶段:半导体2H和金属1T'.
  • 这些相之间的能量差异很小,使MoTe2成为相位工程应用的有希望的候选者.

研究的目的:

  • 研究和控制MoTe2从1T'到2H阶段的固态转化.
  • 实现单晶2H-MoTe2的大规模合成并创建新的异构结构.

主要方法:

  • 密度函数理论 (DFT) 的计算.
  • 传输电子显微镜 (TEM).
  • 能量分散式X射线光谱 (EDS),X射线光电子光谱 (XPS) 和拉曼光谱.
  • 时间-温度转换 (TTT) 图分析.

主要成果:

  • 证明了从多晶1T'-MoTe2到单晶2H-MoTe2的固态相变.
  • 合成大域单晶2H-MoTe2 (直径高达2.34毫米) 和厘米尺度的薄膜.
  • 制造无1T'-2H MoTe2共平面同位点,为二维半导体提供欧姆接触解决方案.

结论:

  • 控制的固体到固体相位转换是晶圆尺度单晶二维半导体的可行途径.
  • 这种方法可以为2D集成电路创建共平面异面结构.
  • 合成的MoTe2同位连接显示了在2D设备中改善电气接触的潜力.