首页> 外文期刊>Journal of chemical theory and computation: JCTC >Comparison of Reaction Field Schemes for Coupling Continuum Solvation Models with Wave Function Methods for Excitation Energies
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Comparison of Reaction Field Schemes for Coupling Continuum Solvation Models with Wave Function Methods for Excitation Energies

机译:励磁能量波函数方法耦合连续体溶剂化模型的反应场方案的比较

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We address in this work the question to which extend reaction field schemes for correlated wave function methods give accurate excitation energies and, at the same time, physically consistent potential energy surfaces. The performance of the perturbation on energy (PTE), perturbation on energy and density (PTED), and post-SCF reaction field schemes is compared for the algebraic diagrammatic construction through second-order, ADC(2), as electronic structure and the conductor-like screening model COSMO as solvation model. The conditions on reaction field schemes to give physically consistent potential energies surfaces are discussed at the example of 4-(N ,N -dimethylamino)benzonitrile, which is used as a test case to assess the artifacts introduced by state-specific contributions to the effective Hamiltonian. To evaluate the accuracy for excitation energies, we use two benchmark sets with data in gas phase and solution for ππ * and nπ * electronic transitions. The experimental solvatochromic shifts are compared to the corresponding calculated values at the COSMO-ADC(2) level with the PTE scheme within the frozen solvent approximation, PTED with the linear response (LR) and corrected linear response (cLR) and post-SCF with LR schemes and with the approximate coupled-cluster singles and doubles method CC2 combined with COSMO in the post-SCF (LR) scheme. The PTE scheme gives at the COSMO-ADC(2) level less accurate solvent shifts than the PTED(LR), PTED(cLR), and post-SCF(LR) schemes. The most accurate prediction of solvatochromism is obtained with the post-SCF(LR) scheme. In most cases, PTED(cLR) performs similar to post-SCF, although its nonlinear perturbative correction causes problems for potential energy surfaces.
机译:我们在这项工作中解决了相关波函数方法扩展反应场方案的问题,可以提供精确的激励能量,并且同时,物理上一致的潜在能量表面。对能量(PTE)的扰动,对能量和密度(PTED)的扰动以及后SCF反应场方案的性能进行比较,并通过二阶ADC(2)作为电子结构和导体的代数示意图。 - 像溶剂化模型一样屏蔽模型COSMO。在4 - ( N, N-二甲基氨基)苄腈的实施例中讨论了对应于物理一致电位电位表面的反应场方案的条件,其用作测试案例以评估状态引入的伪像 - 特定对有效哈密顿的贡献。为了评估励磁能量的准确性,我们使用两个基准组,其中包含气相数据和ππ*和nπ*电子转换的解决方案。将实验性溶性致铬变换与COSMO-ADC(2)水平的相应计算值进行比较,通过冻结溶剂近似,具有线性响应(LR)和校正的线性响应(CLR)和SCF的校正线性响应LR方案和近似耦合簇单打和双打方法CC2在后SCF(LR)方案中与COSMO相结合。 PTE方案在COSMO-ADC(2)水平上,比PTED(LR),PTED(CLR)和后SCF(LR)方案更低的精确溶剂偏移。用SCF(LR)方案获得了对溶性溶解度的最精确预测。在大多数情况下,PTED(CLR)执行类似于后SCF,尽管其非线性扰动校正导致潜在能量表面的问题。

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