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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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Molecular and Ionic Solids02:54

Molecular and Ionic Solids

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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...
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Biasing of Metal-Semiconductor Junctions01:27

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Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
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Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

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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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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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Quantitative Atomic-Site Analysis of Functional Dopants/Point Defects in Crystalline Materials by Electron-Channeling-Enhanced Microanalysis
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Computational approaches to point defect simulations for semiconductor solid solution alloys.

Kelsey J Mirrielees1, Jonathon N Baker1, Preston C Bowes1

  • 1Department of Materials Science and Engineering, North Carolina State University, Raleigh, North Carolina 27695, USA.

The Journal of Chemical Physics
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Summary
This summary is machine-generated.

This study introduces an interpolation method to approximate defect properties in alloys like AlGaN and BST, reducing computational costs. This approach aids in understanding dopant behavior and defect chemistry in complex semiconductor materials.

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Area of Science:

  • Materials Science
  • Computational Materials Science
  • Solid-State Physics

Background:

  • Studying alloy properties using first-principles methods is computationally intensive, especially for materials with random cation site occupation like AlGaN and BaSrTiO3 (BST).
  • Point defects significantly influence the properties of technologically important alloys such as AlGaN and BST.
  • Explicit simulation of these alloys is often too demanding due to the random distribution of elements on crystallographic sites.

Purpose of the Study:

  • To develop a computationally efficient method for approximating defect properties and concentrations in intermediate alloy compositions.
  • To investigate the behavior of Si and Ge dopants in n-type Al-rich AlGaN, including self-compensating defects.
  • To examine the high-temperature defect chemistry of Mg and Fe in BST.

Main Methods:

  • Utilizing interpolation between end-member compounds as a first approximation for defect properties.
  • Analyzing self-compensating defects, multi-donor vacancy complexes, and DX configurations for Si and Ge dopants in AlGaN.
  • Investigating the variation of defect chemistry for Mg and Fe in BST.

Main Results:

  • Demonstrated the efficacy of interpolation for approximating defect properties in AlGaN and BST alloys.
  • Identified key defect mechanisms influencing dopant behavior in AlGaN.
  • Characterized the high-temperature defect chemistry variations in BST.

Conclusions:

  • The interpolation approach provides a viable and computationally tractable first approximation for defect properties in random solid-solution alloys.
  • This method is broadly applicable to semiconductors and dielectrics where alloy properties are governed by point defects.
  • The findings facilitate a better understanding of dopant incorporation and defect mitigation strategies in advanced materials.