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Related Experiment Video

Updated: Jun 10, 2026

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
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Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids

Published on: May 27, 2020

Embedding theory for excited states.

Yuriy G Khait1, Mark R Hoffmann

  • 1Department of Chemistry, University of North Dakota, Grand Forks, North Dakota 58202-9024, USA.

The Journal of Chemical Physics
|August 7, 2010
PubMed
Summary
This summary is machine-generated.

Density functional theory (DFT)-in-DFT and wave function theory (WFT)-in-DFT embedding methods are formally correct for studying ground and excited states. WFT-in-DFT offers systematic excited-state descriptions for embedded subsystem excitations.

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Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

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Last Updated: Jun 10, 2026

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
08:04

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids

Published on: May 27, 2020

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

Area of Science:

  • Quantum Chemistry
  • Computational Physics
  • Electronic Structure Theory

Background:

  • Embedding theories are crucial for studying large quantum systems by dividing them into subsystems.
  • Density Functional Theory (DFT) and Wave Function Theory (WFT) are leading methods for electronic structure calculations.
  • Accurately describing excited states in complex systems remains a significant challenge.

Purpose of the Study:

  • To formally assess the correctness of DFT-in-DFT and WFT-in-DFT embedding approaches for ground and excited states.
  • To investigate the inherent approximations and systematic improvements in these embedding methods.
  • To explore the potential of WFT-in-DFT for reliable excited-state calculations.

Main Methods:

  • Utilizing the Perdew and Levy embedding technique.
  • Deriving and analyzing the equations of motion for DFT-in-DFT.
  • Formally demonstrating the capabilities of WFT-in-DFT for excited-state properties.

Main Results:

  • Both DFT-in-DFT and WFT-in-DFT embedding methods are formally validated for ground and a subset of excited states.
  • The standard DFT-in-DFT approach yields coupled Euler-Lagrange equations without further approximations.
  • WFT-in-DFT provides a systematic pathway for describing excited states originating from the embedded subsystem.

Conclusions:

  • Embedding theories, specifically DFT-in-DFT and WFT-in-DFT, are rigorously applicable to excited-state investigations.
  • WFT-in-DFT presents a promising avenue for accurate excited-state calculations, particularly when excitations are localized.
  • Further research into practical implementations of WFT-in-DFT for excited states is warranted.