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三重激发态的贝塞耳-萨尔皮特基准

Benchmark of Bethe-Salpeter for Triplet Excited-States.

作者信息

Jacquemin Denis, Duchemin Ivan, Blondel Aymeric, Blase Xavier

机构信息

Laboratoire CEISAM - UMR CNR 6230, Université de Nantes , 2 Rue de la Houssinière, BP 92208, 44322 Nantes Cedex 3, France.

Institut Universitaire de France , 103 bd St. Michel, 75005 Paris Cedex 5, France.

出版信息

J Chem Theory Comput. 2017 Feb 14;13(2):767-783. doi: 10.1021/acs.jctc.6b01169. Epub 2017 Feb 3.

Abstract

We have evaluated the accuracy of the Bethe-Salpeter singlet-triplet transition energies as well as singlet-triplet and triplet-triplet splittings for 20 organic molecules, using as reference the CC3 values determined by Thiel and co-workers with both the TZVP and aug-cc-pVTZ atomic basis sets. Our excitation energies are obtained on the basis of GW quasiparticle energy levels that are self-consistently converged with respect to the starting DFT eigenvalues. In its current form, BSE/GW is often unable to provide a balanced description of both singlet and triplet excited-states. While the singlet-singlet and triplet-triplet energy separations are obtained accurately, triplets are located too close in energy from the ground-state, by typically -0.55 eV when using standard functionals to generate the starting eigenstates. Applying the Tamm-Dancoff approximation upshifts the BSE triplet energies and allows reducing this error to ca. -0.40 eV, while using M06-HF eigenstates allows a further increase and hence a reduction of the error for triplet states, but at the cost of larger errors for the singlet excited-states. At this stage, the most accurate TD-DFT estimates therefore remain competitive for computing singlet-triplet transition energies. Indeed, with M06-2X, irrespective of the application or not of the Tamm-Dancoff approximation and of the selected atomic basis set, the deviations obtained with TD-DFT are rather small.

摘要

我们评估了20个有机分子的贝塞耳-萨尔皮特单重态-三重态跃迁能量以及单重态-三重态和三重态-三重态分裂的准确性,以蒂尔及其同事使用TZVP和aug-cc-pVTZ原子基组确定的CC3值作为参考。我们的激发能是基于GW准粒子能级获得的,这些能级相对于起始DFT本征值是自洽收敛的。以其当前形式,BSE/GW通常无法对单重态和三重态激发态提供平衡的描述。虽然单重态-单重态和三重态-三重态能量间隔能够准确获得,但三重态与基态的能量距离过近,使用标准泛函生成起始本征态时,通常相差约-0.55 eV。应用塔姆-丹科夫近似会提高BSE三重态能量,并使该误差降低至约-0.40 eV,而使用M06-HF本征态会进一步提高并因此降低三重态的误差,但代价是单重态激发态的误差会更大。在现阶段,因此最准确的TD-DFT估计值在计算单重态-三重态跃迁能量方面仍然具有竞争力。事实上,使用M06-2X,无论是否应用塔姆-丹科夫近似以及所选的原子基组,TD-DFT获得的偏差都相当小。

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