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Related Concept Videos

Metallic Solids02:37

Metallic Solids

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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.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and...
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Metallic bonds are formed between two metal atoms. A simplified model to describe metallic bonding has been developed by Paul Drüde called the “Electron Sea Model”. 
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Imperfections in Crystal Structure: Non-Stoichiometric Defects01:29

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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...
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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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Diffuse scattering in metallic tin polymorphs.

Björn Wehinger1, Alexeï Bosak, Giuseppe Piccolboni

  • 1European Synchrotron Radiation Facility, BP 220 F-38043 Grenoble Cedex 9, France.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|March 5, 2014
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Summary
This summary is machine-generated.

Lattice dynamics of metallic tin polymorphs were studied using diffuse scattering and inelastic X-ray scattering. Density functional theory accurately described phonon behavior and electronic influences in beta-tin and gamma-tin structures.

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Solid-State Physics

Background:

  • Tin exhibits multiple polymorphs, including beta-tin and gamma-tin, with distinct crystal structures.
  • Understanding lattice dynamics is crucial for predicting material properties and phase transitions.

Purpose of the Study:

  • To investigate the lattice dynamics of beta-tin and gamma-tin polymorphs.
  • To elucidate the influence of electronic structure on phonon behavior.
  • To compare the lattice dynamics of different tin phases.

Main Methods:

  • Diffuse scattering
  • Inelastic X-ray scattering (IXS)
  • Density Functional Perturbation Theory (DFPT)

Main Results:

  • Observed strong resemblance in diffuse scattering patterns between beta-tin and gamma-tin, indicating shared structural and electronic characteristics.
  • Identified unusual asymmetry in thermal diffuse scattering for beta-tin due to its non-symmorphic space group.
  • Anomalies in phonon dispersion relations were linked to the significant influence of the electron subsystem on inter-ionic interactions.

Conclusions:

  • DFPT successfully describes the lattice dynamics of both beta-tin and gamma-tin across various momentum transfers.
  • The combined experimental and theoretical approach provides a comprehensive harmonic description of tin's lattice dynamics.
  • The study highlights the interplay between electronic structure and lattice vibrations in metallic tin.