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Related Concept Videos

Ionic Crystal Structures02:42

Ionic Crystal Structures

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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...
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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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Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

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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...
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The Seven Crystal Systems: Overview01:24

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Crystals with various point group symmetries belong to different crystal classes, which are synonymous terms. Despite being in the same class, crystals may have distinct shapes, like cubes and octahedra. There are 32 three-dimensional point groups, all of which are systematically divided into seven crystal systems.The basic cubic crystal system, exemplified by NaCl, features orthogonal vectors (α = β = �� = 90°) of equal lengths (a = b = c). When specific...
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Unit Cells01:18

Unit Cells

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A crystal's internal structure is an orderly array of atoms, ions, or molecules, and the details of this array significantly influence the solid's properties. In a crystal, periodically repeating 'structural motifs' - which could be atoms, molecules, or groups thereof - create a 'space lattice.' This is essentially a three-dimensional, infinite array of points, each surrounded by its neighbors in an identical way, forming the basic structure of the crystal.A 'unit cell' is a theoretical...
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Metallic Solids02:37

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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.
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Influence of Hybrid Perovskite Fabrication Methods on Film Formation, Electronic Structure, and Solar Cell Performance
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Special quasirandom structures for perovskite solid solutions.

Zhijun Jiang1, Yousra Nahas, Bin Xu

  • 1School of Electronic and Information Engineering & State Key Laboratory for Mechanical Behavior of Materials, Xi'an Jiaotong University, Xi'an 710049, People's Republic of China. Physics Department and Institute for Nanoscience and Engineering, University of Arkansas, Fayetteville, AR 72701, USA.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|September 24, 2016
PubMed
Summary
This summary is machine-generated.

Special quasirandom structures (SQS) accurately model disordered perovskite alloys, predicting properties like electrical polarization and phase transitions. These SQS configurations offer a reliable, computationally efficient approach for materials science research.

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Area of Science:

  • Materials Science
  • Solid-State Physics
  • Computational Chemistry

Background:

  • Disordered perovskite solid solutions present significant challenges in materials modeling.
  • Accurate representation of atomic arrangements is crucial for predicting material properties.

Purpose of the Study:

  • To generate and validate Special Quasirandom Structures (SQS) for various perovskite compositions.
  • To assess the efficacy of SQS in predicting diverse physical properties of disordered perovskites.
  • To compare SQS predictions with results from large random supercells.

Main Methods:

  • Generation of SQS configurations for perovskite alloys (A'1-xBx3 and A(B'1-xX)X3) with varying compositions (x=1/2, 1/3, 2/3).
  • Minimization of Cowley parameters for the nearest neighboring shells in SQS.
  • Application of effective Hamiltonian schemes to predict properties using SQS.
  • Comparison of SQS-derived properties with those from large random supercells for compounds like (Ba1-xSrx)TiO3 and Pb(Zr1-xTix)O3.

Main Results:

  • SQS configurations successfully reproduce numerous properties of large random supercells for most disordered perovskite alloys.
  • Predicted properties include electrical polarization, octahedral tiltings, antipolar motions, antiferromagnetism, strain, piezoelectricity, dielectric response, and specific heat.
  • Formation of polar nanoregions (PNRs) in relaxors was also reproduced.
  • Limitations of SQS configurations were identified and explained.

Conclusions:

  • SQS are a powerful tool for simulating disordered perovskite materials, offering a good balance between accuracy and computational cost.
  • SQS can reliably predict a wide range of physical properties below a material-dependent temperature.
  • The study provides insights into the applicability and limitations of SQS in materials design and discovery.