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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.
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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.
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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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Crystal Field Theory
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Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
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Computation of Atmospheric Concentrations of Molecular Clusters from ab initio Thermochemistry
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Atomic clusters with addressable complexity.

David J Wales1

  • 1University Chemical Laboratories, Lensfield Road, Cambridge CB2 1EW, United Kingdom.

The Journal of Chemical Physics
|February 10, 2017
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Summary
This summary is machine-generated.

This study introduces a method to design atomic clusters that self-organize into desired structures by modifying interatomic potentials. The approach allows for the creation of addressable atomic clusters and their assemblies, like rings and chains.

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Area of Science:

  • Computational chemistry
  • Materials science
  • Statistical mechanics

Background:

  • Designing atomic clusters with specific structures is challenging.
  • Controlling self-assembly requires precise manipulation of potential energy landscapes.

Purpose of the Study:

  • To develop a general formulation for constructing addressable atomic clusters.
  • To enable efficient self-organization of clusters into target structures.
  • To create methods for assembling multiple target clusters.

Main Methods:

  • Modifying interatomic potential well depths to favor nearest-neighbor interactions from reference structures.
  • Biasing the potential energy landscape to create a specific permutational isomer as the global minimum.
  • Introducing repulsive terms between addressed particles to maintain distinguishable targets in assemblies.

Main Results:

  • A framework for designing self-organizing atomic clusters is presented.
  • The method successfully creates addressable clusters, demonstrated for small and large systems (e.g., 55-particle clusters).
  • Visualizations using disconnectivity graphs and identification of biminima aid in understanding complex energy landscapes.
  • Assemblies of target clusters, including rings and chains, can be formed by tuning repulsive interactions.

Conclusions:

  • The developed formulation provides a systematic way to engineer atomic clusters with desired structures.
  • The approach facilitates the creation of addressable clusters and controlled assembly of multiple units.
  • This work offers a powerful tool for designing complex nanostructures through self-assembly.