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The Quantum-Mechanical Model of an Atom02:45

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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.
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An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
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Electron configurations and orbital diagrams can be determined by applying the Aufbau principle (each added electron occupies the subshell of lowest energy available), Pauli exclusion principle (no two electrons can have the same set of four quantum numbers), and Hund’s rule of maximum multiplicity (whenever possible, electrons retain unpaired spins in degenerate orbitals).
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Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
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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...
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Ideally, an unpaired electron shows a single peak in the EPR spectrum due to the transition between the two spin energy states. However, coupling interactions can occur between the spins of the unpaired electron and any neighboring spin-active nuclei. This hyperfine coupling results in hyperfine splitting, where the EPR signal is split into multiplets. The signals split into 2nI + 1 peaks, where n is the number of equivalent nuclei and I is the nuclear spin. These splitting patterns provide...
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How well do one-electron self-interaction-correction methods perform for systems with fractional electrons?

Rajendra R Zope1, Yoh Yamamoto1, Tunna Baruah1

  • 1Department of Physics, The University of Texas at El Paso, El Paso, Texas 79968, USA.

The Journal of Chemical Physics
|February 22, 2024
PubMed
Summary
This summary is machine-generated.

The locally scaled self-interaction correction (LSIC) method shows improved accuracy over the Perdew-Zunger self-interaction correction (PZSIC) method in addressing delocalization errors in electronic structure calculations. Both methods reduce errors, but LSIC offers superior performance in several key areas.

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Area of Science:

  • Quantum Chemistry
  • Computational Materials Science
  • Electronic Structure Theory

Background:

  • Self-interaction error is a significant problem in density functional theory (DFT) approximations.
  • The Perdew-Zunger self-interaction correction (PZSIC) method attempts to correct this error but exhibits paradoxical behavior.
  • The locally scaled self-interaction correction (LSIC) is a newer, one-electron SIC method designed to improve upon PZSIC.

Purpose of the Study:

  • To evaluate the performance of the LSIC method in mitigating delocalization errors.
  • To compare the accuracy of LSIC against PZSIC for various electronic structure problems.
  • To assess the ability of LSIC to describe molecular dissociation and fractional charges.

Main Methods:

  • The study employed the LSIC method with a ratio of kinetic energy densities (zσ) as an iso-orbital indicator.
  • Calculations were performed for molecular dissociation (H2+, He2+, LiF) and vertical ionization energies.
  • The linearity of energy versus electron number curves for fractional charges was analyzed.

Main Results:

  • Both LSIC and PZSIC accurately describe the dissociation of H2+ and He2+, with LSIC showing higher overall accuracy.
  • Neither LSIC nor PZSIC exhibited delocalization errors for the vertical ionization energy of isolated He atoms.
  • Both methods significantly reduced deviations from linearity for fractional charges, with PZSIC being superior for C, Ne, and Ar.
  • LSIC demonstrated accurate charge transfer in LiF dissociation, aligning with experimental and ab initio data.

Conclusions:

  • The LSIC method substantially reduces delocalization errors in electronic structure calculations.
  • LSIC offers improved accuracy and better description of charge transfer compared to PZSIC in specific cases.
  • LSIC shows promise as a robust method for accurate electronic structure predictions.