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Related Concept Videos

Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

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...
Imperfections in Crystal Structure: Non-Stoichiometric Defects01:29

Imperfections in Crystal Structure: Non-Stoichiometric Defects

Non-stoichiometric defects refer to a type of defect in the crystal structure of a compound where the ratio of its constituent elements deviates from the ideal stoichiometric ratio. There are two main types of non-stoichiometric defects: metal excess defects and metal deficiency defects.Metal excess defects occur when there is a slight surplus of metal ions than what is required by the stoichiometric ratio of the compound. For example, heating a sodium chloride crystal in sodium vapor results...
Imperfections in Crystal Structure: Point, Line and Plane Defects01:25

Imperfections in Crystal Structure: Point, Line and Plane Defects

A perfect crystal, in theory, has a uniform structure with the same unit cell and lattice points throughout. However, any deviation from this periodic arrangement is known as an imperfection or defect. These defects can be categorized into three types: point, line, and plane defects.Point defects occur when there is a deviation from the ideal due to missing atoms, displaced atoms, or additional atoms. These imperfections might occur due to imperfect packing during crystallization or because of...
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

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 semiconductor's...
Fermi Level Dynamics01:12

Fermi Level Dynamics

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Types of Semiconductors01:20

Types of Semiconductors

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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Comprehensive Characterization of Extended Defects in Semiconductor Materials by a Scanning Electron Microscope
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Native defects in oxide semiconductors: a density functional approach.

Fumiyasu Oba1, Minseok Choi, Atsushi Togo

  • 1Department of Materials Science and Engineering, Kyoto University, Sakyo, Kyoto 606-8501, Japan. oba@cms.mtl.kyoto-u.ac.jp

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|March 10, 2011
PubMed
Summary
This summary is machine-generated.

This study investigates native defects in oxide semiconductors like ZnO, SrTiO3, and SnO. For ZnO, hydrogen impurities, not native defects, likely cause n-type conductivity, while Ti antisites are key in SrTiO3.

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Area of Science:

  • Materials Science
  • Solid-State Physics
  • Computational Chemistry

Background:

  • Native defects significantly influence the electrical and optical properties of oxide semiconductors.
  • Understanding these defects is crucial for tailoring material functionalities.

Purpose of the Study:

  • To investigate native defects in ZnO, SrTiO3, and SnO using computational methods.
  • To elucidate the role of specific defects in the conductivity and properties of these oxides.

Main Methods:

  • Semilocal and hybrid Hartree-Fock density functional theory calculations.
  • Analysis of defect formation energies and electronic structures.

Main Results:

  • In ZnO, Zn interstitials are shallow donors, while O vacancies create deep states; H impurities are suggested as the source of n-type conductivity.
  • Ti antisites in SrTiO3, alongside O vacancies, explain observed optical and ferroelectric properties.
  • Sn vacancies in SnO act as shallow acceptors, contributing to p-type conductivity.

Conclusions:

  • Native defects play complex roles, with specific defects like H in ZnO and Ti antisites in SrTiO3 being critical.
  • Computational studies provide essential insights into defect behavior and material properties.
  • Defect engineering remains a key strategy for developing advanced oxide semiconductor devices.