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Absorption, resonance, and near‐resonance Raman studies of the tetracyanoquinodimethane neutral and its monoanion in terms of density functional theory and complete active space self‐consistent field methods
Author(s) -
Makowski Marcin,
Pawlikowski Marek T.
Publication year - 2006
Publication title -
international journal of quantum chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.484
H-Index - 105
eISSN - 1097-461X
pISSN - 0020-7608
DOI - 10.1002/qua.20941
Subject(s) - complete active space , excited state , chemistry , resonance (particle physics) , raman spectroscopy , density functional theory , tetracyanoquinodimethane , atomic physics , excitation , field (mathematics) , ground state , resonance raman spectroscopy , space (punctuation) , configuration interaction , basis set , molecular physics , computational chemistry , molecule , physics , quantum mechanics , linguistics , mathematics , philosophy , organic chemistry , pure mathematics
Abstract The electronic structure of the 1 1 B 1u and 1 2 B 3u excited electronic states of the tetracyanoquinodimethane (TCNQ) neutral and its charged derivative are studied within the framework of complete active space self‐consistent field (CASSCF) and Becke's three‐parameter hybrid method with Lee–Yang–Parr correlation functional (B3LYP) methods applied to the level aug‐cc‐p‐VDZ basis set. Both CASSCF/aug‐cc‐p‐VDZ and B3LYP/aug‐cc‐p‐VDZ treatments provide the ground‐state and the excited state geometries; these are then used to assess the Franck–Condon (FC) parameters in the 1 1 B 1u state of the neutral TCNQ and in the 1 2 B 3u state of the TCNQ monoanion. The quality of numerical results is then tested on the base of available experimental near‐resonance and resonance Raman data. The studies are performed in terms of the vibronic model, which takes both FC and mode‐mixing (Dushinsky) effects into account. This somewhat simplified vibronic model leads to very good agreement between the theory and the Raman experiments concerning both neutral TCNQ and its monoanion. In particular, the calculated excitation profiles of the ν 2 = 2215 cm −1 , ν 4 = 1389 cm −1 , ν 5 = 1195 cm −1 , and ν 9 = 336 cm −1 fundamentals are shown to be in excellent agreement with those for the TCNQ monoanion. © 2006 Wiley Periodicals, Inc. Int J Quantum Chem, 2006