Abstract:The
search for new models rapidly delivering accurate excited-state
energies and properties is one of the most active research lines of
theoretical chemistry. Along with these developments, the performance
of known methods is constantly reassessed on the basis of new benchmark
values. In this Letter, we show that the third-order algebraic diagrammatic
construction, ADC(3), does not yield transition energies of the same
quality as the third-order coupled cluster method, CC3. This is demonstrated
by extensive co… Show more
“…58 The accuracy of CC2 and ADC(2) for excitation energies of organic molecules was extensively benchmarked in comparison with more accurate methods, such as CC3 and CCSDT. [59][60][61][62] A mean absolute error of ≈ 0. 22 eV for low-lying singlet states and ≈ 0.12 eV for low-lying triplet states has been estimated.…”
It has recently been shown that cycl[3.3.3]azine and heptazine (1,3,4,6,7,9,9b-heptaazaphenalene) as well as related azaphenalenes exhibit inverted singlet and triplet states, that is, the energy of the lowest singlet excited...
“…58 The accuracy of CC2 and ADC(2) for excitation energies of organic molecules was extensively benchmarked in comparison with more accurate methods, such as CC3 and CCSDT. [59][60][61][62] A mean absolute error of ≈ 0. 22 eV for low-lying singlet states and ≈ 0.12 eV for low-lying triplet states has been estimated.…”
It has recently been shown that cycl[3.3.3]azine and heptazine (1,3,4,6,7,9,9b-heptaazaphenalene) as well as related azaphenalenes exhibit inverted singlet and triplet states, that is, the energy of the lowest singlet excited...
“…These will be our reference as they are known to be extremely accurate (0.03-0.04 eV from the TBEs). [30][31][32]83 Errors associated with these excitation energies (with respect to CC3) are represented in Fig. 2.…”
Section: ��� �mentioning
confidence: 99%
“…46 and 47, we consider here as reference high-level CC calculations performed with the very same geometries and basis sets than our BSE calculations. As pointed out in previous works, [83][84][85] a direct comparison between theoretical transition energies and experimental data is a delicate task, as many factors (such as zero-point vibrational energies and geometrical relaxation) must be taken into account for fair comparisons. Further investigations are required to better evaluate the impact of these considerations on the influence of dynamical screening.…”
The Bethe-Salpeter equation (BSE) formalism is a computationally affordable method for the calculation of accurate optical excitation energies in molecular systems. Similar to the ubiquitous adiabatic approximation of time-dependent density-functional theory, the static approximation, which substitutes a dynamical (i.e., frequency-dependent) kernel by its static limit, is usually enforced in most implementations of the BSE formalism. Here, going beyond the static approximation, we compute the dynamical correction of the electron-hole screening for molecular excitation energies thanks to a renormalized first-order perturbative correction to the static BSE excitation energies. The present dynamical correction goes beyond the plasmon-pole approximation as the dynamical screening of the Coulomb interaction is computed exactly within the random-phase approximation. Our calculations are benchmarked against high-level (coupled-cluster) calculations, allowing to assess the clear improvement brought by the dynamical correction for both singlet and triplet optical transitions.
“…Time-dependent density-functional theory (TD-DFT) has been the dominant force in the calculation of excitation energies of molecular systems in the last two decades. [1][2][3] At a moderate computational cost (at least compared to the other excited-state ab initio methods), TD-DFT can provide accurate transition energies for low-lying excited states of organic molecules (see, for example, Ref. 4 and references therein).…”
Gross-Oliveira-Kohn (GOK) ensemble density-functional theory (GOK-DFT) is a time-independent extension of density-functional theory (DFT) which allows to compute excited-state energies via the derivatives of the ensemble energy with respect to the ensemble weights. Contrary to the time-dependent version of DFT (TD-DFT), double excitations can be easily computed within GOK-DFT. However, to take full advantage of this formalism, one must have access to a weight-dependent exchange-correlation functional in order to model the infamous ensemble derivative contribution to the excitation energies. In the present article, we discuss the construction of first-rung (i.e., local) weightdependent exchange-correlation density-functional approximations for two-electron atomic and molecular systems (He and H 2 ) specifically designed for the computation of double excitations within GOK-DFT. In the spirit of optimally-tuned range-separated hybrid functionals, a two-step system-dependent procedure is proposed to obtain accurate energies associated with double excitations.
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