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Assessment of TD‐DFT‐ and TD‐HF‐based approaches for the prediction of exciton coupling parameters, potential energy curves, and electronic characters of electronically excited aggregates
Author(s) -
Liu Wenlan,
Settels Volker,
Harbach Philipp H. P.,
Dreuw Andreas,
Fink Reinhold F.,
Engels Bernd
Publication year - 2011
Publication title -
journal of computational chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.907
H-Index - 188
eISSN - 1096-987X
pISSN - 0192-8651
DOI - 10.1002/jcc.21781
Subject(s) - excited state , chemistry , coupled cluster , exciton , intermolecular force , density functional theory , potential energy , atomic physics , dipole , scaling , molecular physics , computational chemistry , physics , quantum mechanics , molecule , geometry , mathematics , organic chemistry
The reliability of linear response approaches such as time‐dependent Hartree–Fock (TD‐HF) and time‐dependent density functional theory (TD‐DFT) for the prediction of the excited state properties of 3,4;9,10‐tetracarboxylic‐perylene‐bisimide (PBI) aggregates is investigated. A dimer model of PBI is investigated as a function of a torsional motion of the monomers, which was shown before to be an important intermolecular coordinate in these aggregates. The potential energy curves of the ground state and the two energetically lowest neutral excited and charge‐transfer (CT) states were obtained with the spin‐component scaling modification of the approximate coupled‐cluster singles‐and‐doubles (SCS‐CC2) method as a benchmark for dispersion corrected TD‐HF and a range of TD‐DFT approaches. The highly accurate SCS‐CC2 results are used to assess the other, computationally less demanding methods. TD‐HF predicts similar potential energy curves and transition dipole moments as SCS‐CC2, as well as the correct order of neutral and CT states. This supports an exciton trapping mechanism, which was found on the basis of TD‐HF data. However, the investigated TD‐DFT methods provide generally the opposite character for the excited states. As a consequence, these TD‐DFT results have unacceptably large errors for optical properties of these dye aggregates. © 2011 Wiley Periodicals, Inc. J Comput Chem 2011