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Related Concept Videos

The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra. Schrödinger...
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Tetrahedral Complexes
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,...
Valence Bond Theory and Hybridized Orbitals02:38

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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.
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Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as the nucleus...
IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration01:16

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A covalently bonded heteronuclear diatomic molecule can be modeled as two vibrating masses connected by a spring. The vibrational frequency of the bond can be expressed using an equation derived from Hooke's law, which describes how the force applied to stretch or compress a spring is proportional to the displacement of the spring. In this case, the atoms behave like masses, and the bond acts like a spring.
According to Hooke's law, the vibrational frequency is directly proportional to the...

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Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
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Rydberg energies using excited state density functional theory.

Chiao-Lun Cheng1, Qin Wu, Troy Van Voorhis

  • 1Department of Chemistry, Massachusetts Institute of Technology, 77 Massachusetts Ave., Cambridge, Massachusetts 02139, USA.

The Journal of Chemical Physics
|December 3, 2008
PubMed
Summary

Excited state density functional theory (eDFT) accurately calculates Rydberg energies in atoms, outperforming time-dependent DFT. This method uses excited state densities for accurate Kohn-Sham potentials, offering a rigorous approach for specific quantum systems.

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Area of Science:

  • Quantum Chemistry
  • Computational Physics
  • Theoretical Chemistry

Background:

  • Accurate calculation of atomic Rydberg states is crucial for understanding electronic structure.
  • Traditional time-dependent density functional theory (TDDFT) often fails for Rydberg states.
  • Excited state density functional theory (eDFT) presents an alternative computational approach.

Purpose of the Study:

  • To investigate the efficacy of excited state density functional theory (eDFT) for calculating Rydberg states in atoms.
  • To compare eDFT performance against time-dependent density functional theory (TDDFT).
  • To explore the theoretical underpinnings and limitations of eDFT for these systems.

Main Methods:

  • Utilized excited state density functional theory (eDFT) with semilocal functionals.
  • Employed analytical and numerical methods to study Rydberg energies.
  • Applied optimized effective potential (OEP) techniques to analyze density v-representability.

Main Results:

  • eDFT, using semilocal functionals, yielded accurate Rydberg energies, succeeding where TDDFT failed.
  • The Kohn-Sham potential in eDFT, derived from excited state densities, exhibits polynomial decay, enabling Rydberg series.
  • eDFT solutions are rigorous when the excited state density minimizes non-interacting kinetic energy.

Conclusions:

  • eDFT provides a robust and accurate method for studying atomic Rydberg states.
  • The success of eDFT stems from its use of state-specific potentials derived from excited state densities.
  • eDFT complements constrained DFT, offering a rigorous framework for non-ground-state densities.