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Updated: Oct 4, 2025

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Published on: May 27, 2020
Full-frequency dynamical Bethe-Salpeter equation without frequency and a study of double excitations
Sylvia J Bintrim1, Timothy C Berkelbach1
1Department of Chemistry, Columbia University, New York, New York 10027, USA.
This study reformulates the frequency-dependent Bethe-Salpeter equation (BSE) into a frequency-independent problem, reducing computational cost from O(N^6) to O(N^5). This method accurately captures double excitation character in excited states.
Area of Science:
- Computational chemistry
- Quantum mechanics
- Electronic structure theory
Background:
- The GW approximation combined with the Bethe-Salpeter equation (BSE) is a standard method for calculating electronic excitations.
- The computational cost of the full-frequency dynamical BSE is prohibitively high (O(N^6)) due to the frequency-dependent screened Coulomb interaction.
Purpose of the Study:
- To reformulate the full-frequency dynamical BSE into a computationally tractable form.
- To enable accurate calculations of excited states, including those with significant double excitation character.
Main Methods:
- Reformulation of the dynamical BSE as a frequency-independent eigenvalue problem in an expanded space.
- Application of iterative eigensolvers and density fitting approximations.
- Numerical verification of the O(N^5) computational scaling.
Main Results:
- Achieved an O(N^5) computational scaling for the dynamical BSE, significantly reducing computational cost.
- Developed a method that provides direct access to excited states with dominant double excitation character.
- Demonstrated that the GW/BSE method overestimates excitation energies and underestimates double excitation character for the 2^1Ag states of polyenes.
Conclusions:
- The reformulated dynamical BSE offers a computationally efficient and accurate approach for electronic excitation calculations.
- The method overcomes limitations of the static screening approximation by including full-frequency dependence.
- This advancement is crucial for accurately describing excited states with complex electronic character.
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