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Related Concept Videos

Crystal Field Theory - Octahedral Complexes02:58

Crystal Field Theory - Octahedral Complexes

Crystal Field Theory
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.
CFT focuses on...
Determination of Crystal Structures01:29

Determination of Crystal Structures

In the late 1800s, the revelation that light extended beyond visible wavelengths led to the discovery of X-rays by Wilhelm Roentgen. Recognized as high-energy electromagnetic radiation with short wavelengths, X-rays prompted exploration into their interaction with crystals. Max von Laue proposed in 1912 that the periodic arrangement of atoms, ions, or molecules in crystals would cause them to diffract X-rays, a hypothesis confirmed through experiments with copper sulfate and zinc sulfide...
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,...
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...
Crystal Growth: Principles of Crystallization01:25

Crystal Growth: Principles of Crystallization

Crystallization is a phase transformation process in which crystals are precipitated from a supersaturated solution or formed from other sources. During crystallization, atoms or molecules arrange themselves into a well-defined, rigid crystal lattice to minimize energy.
Initiating crystallization involves manipulating the concentration of the solute and the temperature of the solution. Since crystal growth occurs when the ratio of concentration and solubility of the solute in the solvent – the...

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Functionalization of Single-walled Carbon Nanotubes with Thermo-reversible Block Copolymers and Characterization by Small-angle Neutron Scattering
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Crystal structure transfer in core/shell nanowires.

Rienk E Algra1, Moïra Hocevar, Marcel A Verheijen

  • 1Materials Innovation Institute (M2i), 2628CD Delft, The Netherlands.

Nano Letters
|March 23, 2011
PubMed
Summary

Researchers engineered silicon (Si) nanotubes with controlled crystal structures by transferring a twinning superlattice from a gallium phosphide core. This breakthrough enables precise tuning of opto-electronic properties in Si nanowires for advanced semiconductor applications.

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Area of Science:

  • Semiconductor science and engineering
  • Materials science
  • Nanotechnology

Background:

  • Structure engineering is crucial for controlling semiconductor opto-electronic properties.
  • Twinning superlattices have been achieved in III-V nanowires but not in silicon (Si) nanowires.
  • Si nanowires are vital for the semiconductor industry.

Purpose of the Study:

  • To develop a method for controlling the crystal structure of Si nanowires.
  • To enable the formation of twinning superlattices in Si nanowires.
  • To precisely tune the opto-electronic properties of Si-based nanostructures.

Main Methods:

  • Epitaxial growth of a silicon shell onto a gallium phosphide (GaP) core wire.
  • Transfer of a designed twinning superlattice (zinc blende or wurtzite structure) from the GaP core to the Si shell.
  • Utilizing the small lattice mismatch (0.4%) between GaP and Si for defect-free structure transfer.
  • Selective wet-chemical etching of the GaP core to yield free-standing Si nanotubes.

Main Results:

  • Successful transfer of twinning superlattices from GaP to Si, creating novel Si nanostructures.
  • Demonstrated precise control over superlattice periodicity and Si shell thickness.
  • Fabricated arrays of free-standing silicon nanotubes with engineered crystal structures.

Conclusions:

  • This approach provides unprecedented control over the crystal structure of Si nanowires and nanotubes.
  • The developed method allows for defect-free transfer of superlattices, enabling tunable opto-electronic properties.
  • The resulting Si nanotubes are promising for next-generation semiconductor devices.