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Related Concept Videos

Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

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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,...
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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.
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To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
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The size of the unit cell and the arrangement of atoms in a crystal may be determined from measurements of the diffraction of X-rays by the crystal, termed X-ray crystallography.
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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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Related Experiment Video

Updated: Oct 7, 2025

Sample Preparation and Transfer Protocol for In-Vacuum Long-Wavelength Crystallography on Beamline I23 at Diamond Light Source
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A symmetry-orientated divide-and-conquer method for crystal structure prediction.

Xuecheng Shao1, Jian Lv1, Peng Liu1

  • 1International Center of Computational Method and Software, College of Physics, Jilin University, Changchun 130012, China.

The Journal of Chemical Physics
|January 9, 2022
PubMed
Summary

This study introduces a novel symmetry-based method to simplify crystal structure prediction. The approach efficiently explores complex structures by focusing on high-symmetry subspaces, accelerating the discovery of new materials.

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Area of Science:

  • Materials Science
  • Computational Chemistry
  • Crystallography

Background:

  • Crystal structure prediction is crucial for materials discovery but computationally challenging due to high-dimensional potential energy surfaces.
  • Existing methods struggle with complex structures and preserving crystal symmetry during exploration.

Purpose of the Study:

  • To develop a novel, efficient, and symmetry-aware method for predicting complex crystal structures.
  • To simplify the global minimization problem in crystal structure prediction.

Main Methods:

  • A symmetry-orientated divide-and-conquer scheme to construct a symmetry tree graph.
  • Decomposition of the search space into symmetry-dependent subspaces.
  • An artificial intelligence-based symmetry selection strategy to explore low-lying, high-symmetry subspaces.

Main Results:

  • Successfully predicted candidate structures for binary Lennard-Jones mixtures.
  • Accurately predicted the high-pressure phase of ice with over 100 atoms.
  • Demonstrated simplification of crystal structure prediction by avoiding the complex P1 subspace.

Conclusions:

  • The proposed method effectively predicts complex crystal structures by leveraging symmetry.
  • This approach offers a significant advancement towards achieving reliable crystal structure prediction for complex systems.
  • Preserves crystal symmetry throughout the structure evolution process.