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Imagine a bucket of water. It contains many molecules, of the order of 1026 molecules. Thus, although it contains discrete elements (molecules) at the microscopic level, macroscopically, it can be considered continuous. Small volume elements of water, infinitesimal compared to the bulk of the bucket's volume, still contain many molecules. Under this framework, quantized matter is approximated as continuous for practical purposes.
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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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Perturbative ensemble density functional theory applied to charge transfer excitations.

Gil S Amoyal1, Leeor Kronik1, Tim Gould2

  • 1Department of Molecular Chemistry and Materials Science, Weizmann Institute of Sciences, Perlman Chemical Sciences Building, Rehovoth, 76100, ISRAEL.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|December 17, 2024
PubMed
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Perturbative ensemble DFT (pEDFT) offers a low-cost method for calculating charge transfer excitation energies. While qualitatively correct, pEDFT is less quantitatively accurate than time-dependent DFT due to self-interaction errors.

Keywords:
Charge transfer excitationsEnsemble density functional theoryself-interaction error

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Area of Science:

  • Quantum Chemistry
  • Computational Chemistry
  • Theoretical Chemistry

Background:

  • Charge transfer excitation energies pose challenges for standard time-dependent density functional theory (TDDFT).
  • Perturbative ensemble DFT (pEDFT) is a proposed low-cost, in-principle exact alternative for excitation energy calculations.
  • pEDFT has shown promise for valence excitation energies.

Purpose of the Study:

  • To analytically and numerically evaluate the performance of pEDFT for charge transfer excitation energies.
  • To compare pEDFT's accuracy against TDDFT in the charge transfer limit.
  • To identify factors limiting pEDFT's quantitative accuracy.

Main Methods:

  • Analytical examination of pEDFT in the charge transfer limit.
  • Numerical calculations using the benzene-tetracyanoethylene complex.
  • Comparison of pEDFT results with TDDFT benchmarks.

Main Results:

  • pEDFT qualitatively captures the Mulliken limit for charge transfer excitation energies.
  • pEDFT's performance shows weak dependence on the choice of density functional approximation.
  • Quantitative accuracy of pEDFT is found to be lower than TDDFT.
  • A novel self-interaction-like term emerges in pEDFT, negatively impacting accuracy.

Conclusions:

  • pEDFT is a qualitatively useful method for charge transfer excitation energies.
  • Quantitative improvements are needed to match TDDFT accuracy.
  • Understanding and mitigating the new self-interaction term is crucial for advancing pEDFT.