2018
DOI: 10.1021/acs.jctc.7b01013
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Accurate Evaluation of Real-Time Density Functional Theory Providing Access to Challenging Electron Dynamics

Abstract: We demonstrate that electronic excitations and their transition densities can be obtained from real-time density functional theory calculations with great accuracy by relating the data from numerical propagation to the analytical form of the electronic response after a boost excitation. The latter is derived in this article. This approach facilitates quantitatively obtaining oscillator strengths, identifying excitations that carry very small oscillator strengths, and assessing electronic couplings from transit… Show more

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Cited by 36 publications
(34 citation statements)
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“…We extract the optical absorption cross section matrix Σ ij at the energy of the transition B, and we diagonalize it. For a nondegenerate band, we expect just one eigenvalue different from zero, and since , 22,34 the normalized eigenvector associated with the nonzero eigenvalue would set the direction for the TDM, d 0B . If in turn the band is almost degenerate, we can still find the TDMs with the largest contributions to the absorption by diagonalizing the cross-section matrix and taking the eigenvectors associated with the highest eigenvalues.…”
Section: Resultsmentioning
confidence: 99%
“…We extract the optical absorption cross section matrix Σ ij at the energy of the transition B, and we diagonalize it. For a nondegenerate band, we expect just one eigenvalue different from zero, and since , 22,34 the normalized eigenvector associated with the nonzero eigenvalue would set the direction for the TDM, d 0B . If in turn the band is almost degenerate, we can still find the TDMs with the largest contributions to the absorption by diagonalizing the cross-section matrix and taking the eigenvectors associated with the highest eigenvalues.…”
Section: Resultsmentioning
confidence: 99%
“…All calculations for the H 8 −H 8 charge-transfer system were performed spin polarized, self-consistently on a realspace grid with BTDFT [40] using Troullier-Martins LDA pseudopotentials [137], ellipsoidal boundaries with semiaxis of 20a 0 perpendicular to and 32a 0 along the chains, and a grid spacing of 0.3a 0 . For the KS iterations, an energy convergence criterion of 5 × 10 −6 E h was used.…”
Section: Appendix E: H 8 −H 8 Charge-transfer Calculation Detailsmentioning
confidence: 99%
“…The chromophores in turn are typically embedded in a protein matrix, at least parts of which should also be taken into account explicitly [33,[35][36][37]. However, semilocal functionals are currently at their limits for such systems due to their inability to properly describe charge transfer [38][39][40]. Therefore, there is a serious need for functionals that do not suffer from the large, qualitative errors that traditional semilocal functionals plague, yet come at a comparable computational price.…”
Section: Introductionmentioning
confidence: 99%
“…where δ ρ(r, ω) is the Fourier Transform of the timedependent (TD) induced density δρ(r, t) = ρ(r, t) − ρ(r, 0). Many research groups have recently contributed to this topic [97][98][99][100] , focusing on low-frequency excitations.…”
Section: K Edgementioning
confidence: 99%