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Related Concept Videos

Band Theory02:35

Band Theory

When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
Valence Bond Theory and Hybridized Orbitals02:38

Valence Bond Theory and Hybridized Orbitals

According to valence bond theory, a covalent bond results when: (1) an orbital on one atom overlaps an orbital on a second atom, and (2) the single electrons in each orbital combine to form an electron pair. The strength of a covalent bond depends on the extent of overlap of the orbitals involved. Maximum overlap is possible when the orbitals overlap on a direct line between the two nuclei.
A σ bond (single bond in a Lewis structure) is a covalent bond in which the electron density is...
Hybridization of Atomic Orbitals II03:35

Hybridization of Atomic Orbitals II

sp3d and sp3d 2 Hybridization
The Aufbau Principle and Hund's Rule03:02

The Aufbau Principle and Hund's Rule

To determine the electron configuration for any particular atom, we can build the structures in the order of atomic numbers. Beginning with hydrogen, and continuing across the periods of the periodic table, we add one proton at a time to the nucleus and one electron to the proper subshell until we have described the electron configurations of all the elements. This procedure is called the aufbau principle, from the German word aufbau (“to build up”). Each added electron occupies the subshell of...
Structure of Benzene: Molecular Orbital Model01:18

Structure of Benzene: Molecular Orbital Model

According to the molecular orbital (MO) model, benzene has a planar structure with a regular hexagon of six sp2 hybridized carbons. As shown in Figure 1, each carbon is bonded to three other atoms with C–C–C and H–C–C bond angles of 120°. The C–H bond length is 109 pm, and the C–C bond length is 139 pm which is midway between the single bond length of sp3 hybridized carbons (154 pm) and sp2 hybridized carbons (133 pm).
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...

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Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
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Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations

Published on: October 12, 2019

Hubbard-U band-structure methods.

R C Albers1, N E Christensen, A Svane

  • 1Theoretical Division, Los Alamos National Laboratory, Los Alamos, NM 87545, USA.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|July 1, 2011
PubMed
Summary
This summary is machine-generated.

Electronic-structure calculations using the Hubbard term are increasingly common. However, these methods are better viewed as phenomenological corrections rather than first-principles approaches.

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Area of Science:

  • Condensed Matter Physics
  • Computational Materials Science
  • Quantum Chemistry

Background:

  • The local-density approximation (LDA) is a common starting point for electronic structure calculations.
  • Adding a Hubbard term (e.g., LDA+U) aims to improve descriptions of correlated electron systems.
  • Dynamical Mean-Field Theory (DMFT) offers a more sophisticated many-body approach.

Purpose of the Study:

  • To review the physics behind Hubbard-corrected electronic structure calculations.
  • To critically assess the strengths and weaknesses of these methods.
  • To re-evaluate the theoretical underpinnings and justifications for these calculations.

Main Methods:

  • Review of existing literature on Hubbard-based electronic structure methods.
  • Analysis of the theoretical assumptions versus the practical implementation of these methods.
  • Comparison with first-principles calculations and phenomenological models.

Main Results:

  • Common assumptions justifying Hubbard-corrected calculations are often inconsistent with their actual implementation.
  • These calculations are frequently treated as first-principles, but are argued to be phenomenological.
  • An alternative perspective views them as complex Hubbard models.

Conclusions:

  • Hubbard-corrected electronic structure calculations should be re-conceptualized.
  • They are better understood as phenomenological many-body corrections to band theory.
  • This re-framing impacts the interpretation and application of results in condensed matter physics.