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Force can be calculated from the expression for potential energy, which is a function of position. The component of a conservative force, in a particular direction, equals the negative of the derivative of the corresponding potential energy with respect to the displacement in that direction. For regions where potential energy changes rapidly with displacement, the work done and force is maximum. Also, when force is applied along the positive coordinate axis, the potential energy decreases with...
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In an atom, the negatively charged electrons are attracted to the positively charged nucleus. In a multielectron atom, electron-electron repulsions are also observed. The attractive and repulsive forces are dependent on the distance between the particles, as well as the sign and magnitude of the charges on the individual particles. When the charges on the particles are opposite, they attract each other. If both particles have the same charge, they repel each other.
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Stable molecules exist because covalent bonds hold the atoms together. The strength of a covalent bond is measured by the energy required to break it, that is, the energy necessary to separate the bonded atoms. Separating any pair of bonded atoms requires energy — the stronger a bond, the greater the energy required to break it.
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Atoms and molecules interact through bonds (or forces): intramolecular and intermolecular. The forces are electrostatic as they arise from interactions (attractive or repulsive) between charged species (permanent, partial, or temporary charges) and exist with varying strengths between ions, polar, nonpolar, and neutral molecules. The different types of intermolecular forces are ion–dipole, dipole–dipole, hydrogen bonds, and dispersion; among these, dipole–dipole, hydrogen...
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Exchange energies with forces in density-functional theory.

Nicolas Tancogne-Dejean1, Markus Penz2,3, Andre Laestadius2,4

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We introduce a novel force-based approach for density-functional theory, offering a computationally efficient alternative to energy-based methods for approximating exchange-correlation potentials and energies.

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Area of Science:

  • Quantum Chemistry
  • Computational Physics
  • Materials Science

Background:

  • Density-functional theory (DFT) is a cornerstone for electronic structure calculations.
  • Approximations to exchange-correlation functionals are crucial for DFT accuracy.
  • Current methods often rely on energy functionals, which can be computationally intensive.

Purpose of the Study:

  • To develop a new, computationally efficient route for approximating exchange-correlation potentials and energies in DFT.
  • To explore the use of exact force expressions as an alternative to energy functionals.
  • To establish a framework for developing nonlocal and nonadiabatic approximations.

Main Methods:

  • Replacing energy functionals with physically equivalent exact force expressions.
  • Splitting force differences into Hartree, exchange, and correlation components.
  • Solving a Poisson equation for scalar potentials and utilizing transverse forces for vector potentials.

Main Results:

  • The force-based method yields scalar and vector potentials, with vector potentials satisfying exact constraints.
  • The force-based local-exchange potential and energy show good agreement with the optimized effective potential method.
  • This approach offers a promising alternative to traditional energy-based methods.

Conclusions:

  • The force-based approach provides a numerically inexpensive and effective route for DFT approximations.
  • It opens avenues for developing advanced, computationally tractable nonlocal and nonadiabatic approximations.
  • This method has significant implications for advancing electronic structure calculations.