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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...
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...
Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

Crystal Field Theory - Tetrahedral and Square Planar Complexes

Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
Crystallographic Point Groups01:29

Crystallographic Point Groups

Crystallographic point groups represent the various symmetry operations that can occur within crystals. They are unique in that at least one point will always remain unchanged during these actions. For instance, consider the triclinic system. This system, devoid of any axis or plane of symmetry, aligns with the C1 and Ci point groups.where Cᵢ is characterized solely by a center of inversion.Contrastingly, the monoclinic system introduces an element of symmetry. This system with one plane and...
Unit Cells01:18

Unit Cells

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...
VSEPR Theory and the Effect of Lone Pairs04:01

VSEPR Theory and the Effect of Lone Pairs

Effect of Lone Pairs of Electrons on Molecule Geometry

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Updated: Jun 13, 2026

Demonstrating the Simplicity and In Situ Temperature Monitoring of the Mechanochemical Synthesis of Metal Chalcogenides Suitable for Thermoelectrics
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Monoclinic Cu2Se3Sn.

L D Gulay1, M Daszkiewicz, T A Ostapyuk

  • 1Department of Ecology and Protection of the Environment, Volyn National University, Voli Avenue 13, 43009 Lutsk, Ukraine.

Acta Crystallographica. Section C, Crystal Structure Communications
|May 6, 2010
PubMed
Summary
This summary is machine-generated.

Researchers discovered a new crystal structure for dicopper(I) triselenostannate(IV), Cu(2)Se(3)Sn. This ordered structure is a superstructure of previously known cubic and monoclinic forms, revealing new insights into solid-state chemistry.

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Area of Science:

  • Solid State Chemistry
  • Inorganic Chemistry
  • Crystallography

Background:

  • Dicopper(I) triselenostannate(IV), Cu(2)Se(3)Sn, is a complex inorganic compound.
  • Previous studies identified cubic and monoclinic modifications of Cu(2)Se(3)Sn.
  • These modifications exhibit varying degrees of order in atom distribution.

Purpose of the Study:

  • To synthesize and characterize a previously unknown modification of dicopper(I) triselenostannate(IV).
  • To elucidate the crystal structure and atomic arrangement of this new phase.
  • To compare the new structure with existing modifications of Cu(2)Se(3)Sn.

Main Methods:

  • Synthesis from the Cu(2)Se-SnSe(2) quasi-binary system.
  • Investigation using X-ray single-crystal diffraction.
  • Analysis of atomic positions and symmetry.

Main Results:

  • A novel modification of dicopper(I) triselenostannate(IV), Cu(2)Se(3)Sn, was successfully obtained.
  • The crystal structure features a closest-packed arrangement of selenium atoms (ABC sequence).
  • Copper atoms occupy 1/3 of tetrahedral interstices, and tin atoms occupy 1/6.
  • This new structure is an ordered superstructure of previously reported cubic and monoclinic forms, with 96 atoms per unit cell.

Conclusions:

  • The newly discovered Cu(2)Se(3)Sn modification represents a complex superstructure with ordered cation distribution.
  • This finding expands the understanding of structural polymorphism in ternary selenium-tin compounds.
  • The detailed structural analysis provides a basis for further research into the properties of these materials.