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Related Concept Videos

Metallic Solids02:37

Metallic Solids

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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....
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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...
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Semiconductors01:22

Semiconductors

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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...
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Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

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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...
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Structures of Solids02:22

Structures of Solids

21.1K
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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Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

14.8K
The structure of a crystalline solid, whether a metal or not, is best described by considering its simplest repeating unit, which is referred to as its unit cell. The unit cell consists of lattice points that represent the locations of atoms or ions. The entire structure then consists of this unit cell repeating in three dimensions. The three different types of unit cells present in the cubic lattice are illustrated in Figure 1.
Types of Unit Cells
Imagine taking a large number of identical...
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Fabricating van der Waals Heterostructures with Precise Rotational Alignment
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Topologic connection between 2-D layered structures and 3-D diamond structures for conventional semiconductors.

Jianwei Wang1,2, Yong Zhang1

  • 1Department of Electrical and Computer Engineering, The University of North Carolina at Charlotte 9201 University City Boulevard, Charlotte, NC 28223, USA.

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Researchers explored 3D semiconductors to discover new 2D materials. Applying strain revealed promising new layered structures like GaN and Si, expanding the search beyond traditional layered materials.

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Computational Materials Science

Background:

  • Discovering new 2D materials is crucial for next-generation electronics.
  • Traditionally, 2D materials are sought from layered precursors, but 3D materials offer unexplored potential.

Purpose of the Study:

  • To systematically investigate common Group IV, III-V, and II-VI semiconductors as potential sources for novel 2D materials.
  • To identify new 2D structures derived from 3D parent materials through controlled deformation.

Main Methods:

  • Density Functional Theory (DFT) calculations were employed.
  • Systematic study of Group IV, III-V, and II-VI semiconductors under compressive and tensile strain along symmetry axes.
  • Analysis of total energy changes to identify metastable states and phonon spectra for structural stability.

Main Results:

  • Two major phase transition paths (from wurtzite and NiAs structures) were identified.
  • Tensile strain led to low and high buckled monolayer structures.
  • Promising new 2D materials identified include BeO, GaN, ZnO (tensile strain) and Ge, Si, GaP (compressive strain).

Conclusions:

  • 3D semiconductors can be a viable source for novel 2D materials.
  • Controlled strain engineering is an effective method for discovering new 2D materials.
  • The identified materials hold promise for future electronic and optoelectronic applications.