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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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An ionic compound is stable because of the electrostatic attraction between its positive and negative ions. The lattice energy of a compound is a measure of the strength of this attraction. The lattice energy (ΔHlattice) of an ionic compound is defined as the energy required to separate one mole of the solid into its component gaseous ions. For the ionic solid sodium chloride, the lattice energy is the enthalpy change of the process:
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Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
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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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Triangular lattice exciton model.

Daniel Gunlycke1, Frank Tseng2

  • 1US Naval Research Laboratory, Washington, District of Columbia, USA. daniel.gunlycke@nrl.navy.mil.

Physical Chemistry Chemical Physics : PCCP
|March 8, 2016
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Summary
This summary is machine-generated.

The 2D hydrogen model for excitons fails in transition-metal dichalcogenides due to lattice effects. Excitons in these materials exist in an intermediate regime between Wannier and Frenkel types.

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Quantum Mechanics

Background:

  • Excitons are fundamental quasiparticles in semiconductors, crucial for understanding optical and electronic properties.
  • The standard models for describing excitons include the Wannier and Frenkel models, each with distinct characteristics.
  • Monolayer transition-metal dichalcogenides (TSeCs) exhibit unique excitonic behavior due to their reduced dimensionality and strong spin-orbit coupling.

Purpose of the Study:

  • To investigate the breakdown of the two-dimensional hydrogen model for excitons in semiconducting monolayer TSeCs.
  • To characterize the nature of excitons in these materials, determining if they fit existing models or occupy an intermediate regime.
  • To develop a computationally efficient model for studying excitons in TSeCs.

Main Methods:

  • Development of a minimalistic equilateral triangular lattice model.
  • Formulation of the model in sparse form in direct space.
  • Computational solution of the lattice model.

Main Results:

  • The study explicitly demonstrates the inadequacy of the 2D hydrogen model for excitons in monolayer TSeCs.
  • Lattice effects are identified as the primary reason for the breakdown of the standard model.
  • Excitons in these materials are shown to exist in an intermediate regime, distinct from both pure Wannier and pure Frenkel excitons.

Conclusions:

  • The conventional 2D hydrogen model is insufficient for accurately describing excitons in semiconducting monolayer TSeCs.
  • A novel lattice model provides a more accurate and computationally efficient approach to studying these excitons.
  • The findings necessitate a revised understanding of exciton physics in low-dimensional materials.