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Related Concept Videos

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...
Lattice Centering and Coordination Number02:33

Lattice Centering and Coordination Number

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.
Types of Unit Cells
Imagine taking a large number of identical...
Hybridization of Atomic Orbitals I03:24

Hybridization of Atomic Orbitals I

The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
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...
Exceptions to the Octet Rule02:55

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Many covalent molecules have central atoms that do not have eight electrons in their Lewis structures. These molecules fall into three categories:
VSEPR Theory and the Basic Shapes02:52

VSEPR Theory and the Basic Shapes

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Stacking in bulk and bilayer hexagonal boron nitride.

Gabriel Constantinescu1, Agnieszka Kuc, Thomas Heine

  • 1School of Engineering and Science, Jacobs University Bremen, Campus Ring 1, 28759 Bremen, Germany.

Physical Review Letters
|August 6, 2013
PubMed
Summary
This summary is machine-generated.

High-level ab initio theory reveals AA' stacking is most stable for hexagonal boron nitride bilayers. Electrostatic and London dispersion forces govern interlayer distance, with a low energy barrier for sliding.

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Computational Chemistry

Background:

  • Layered hexagonal boron nitride (h-BN) is a crucial material with unique electronic and mechanical properties.
  • Understanding interlayer interactions is vital for predicting and controlling the behavior of 2D materials.

Purpose of the Study:

  • To investigate the stacking orders and interlayer interactions in hexagonal boron nitride bulk and bilayers.
  • To determine the most stable stacking configuration and the energy barrier for sliding.

Main Methods:

  • Utilized high-level ab initio theory, specifically local second-order Møller-Plesset perturbation theory (LMP2).
  • Analyzed electrostatic and London dispersion interactions contributing to interlayer forces.

Main Results:

  • Identified AA' stacking as the most stable configuration for h-BN bilayers.
  • Quantified the minimum energy sliding path, revealing a low energy barrier of 3.4 meV per atom.
  • Found that standard density functionals often fail to accurately predict interlayer energies, unlike a specific PBE functional.

Conclusions:

  • Electrostatic and London dispersion forces are key drivers of interlayer distance and stacking order in h-BN.
  • The AA' stacking configuration is energetically favored, with minimal energy required for sliding.
  • Accurate theoretical prediction of h-BN interlayer energies requires advanced methods or specific functionals, aligning well with experimental findings.