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Related Concept Videos

Ionic Crystal Structures02:42

Ionic Crystal Structures

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...
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...
Metallic Solids02:37

Metallic Solids

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. Many...
Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

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...
Electron Configuration of Multielectron Atoms03:26

Electron Configuration of Multielectron Atoms

The alkali metal sodium (atomic number 11) has one more electron than the neon atom. This electron must go into the lowest-energy subshell available, the 3s orbital, giving a 1s22s22p63s1 configuration. The electrons occupying the outermost shell orbital(s) (highest value of n) are called valence electrons, and those occupying the inner shell orbitals are called core electrons. Since the core electron shells correspond to noble gas electron configurations, we can abbreviate electron...

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Disordered La3Cu4.88Se7.

L D Gulay1, M Daszkiewicz, O M Strok

  • 1Department of Ecology and Protection of the Environment, Volyn National University, Lutsk, Ukraine.

Acta Crystallographica. Section C, Crystal Structure Communications
|March 4, 2011
PubMed
Summary
This summary is machine-generated.

Researchers studied copper(I) lanthanum selenide, La(3)Cu(4.88)Se(7), revealing a crystal structure with ordered La and Se atoms. Partially occupied copper sites suggest a potential pathway for ionic diffusion.

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Growth and Electrostatic/chemical Properties of Metal/LaAlO3/SrTiO3 Heterostructures
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11:54

Growth and Electrostatic/chemical Properties of Metal/LaAlO3/SrTiO3 Heterostructures

Published on: February 8, 2018

Area of Science:

  • Solid-state chemistry
  • Materials science
  • Crystallography

Background:

  • Lanthanum selenides and copper selenides are important in materials science.
  • Understanding the crystal structure of mixed lanthanum-copper selenides is crucial for their applications.

Purpose of the Study:

  • To determine the crystal structure of copper(I) lanthanum selenide, La(3)Cu(4.88)Se(7).
  • To investigate the atomic arrangement and potential for ionic diffusion within this compound.

Main Methods:

  • X-ray single-crystal diffraction was employed to analyze the crystal structure.
  • Analysis focused on the positions and occupancy of La, Cu, and Se atoms.

Main Results:

  • The crystal structure of La(3)Cu(4.88)Se(7) was elucidated.
  • Lanthanum and selenium atoms occupy ordered positions on mirror planes.
  • Copper atoms exhibit partial occupancy across five distinct crystallographic sites.
  • The structure is composed of edge-sharing [LaSe(6)] and [LaSe(7)] polyhedra.

Conclusions:

  • The partially occupied copper sites create potential pathways for ionic diffusion.
  • The determined crystal structure provides a foundation for understanding the properties and potential applications of this material.