doi:10.1016/j.cplett.2004.11.054
Copyright © 2004 Elsevier B.V. All rights reserved.
The asymmetric nature of charge transfer states of the cyano-substituted proton sponge
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A. Szemik-Hojniaka,
,
, I. Deperasińskab,
, W.J. Bumac,
, G. Balkowskic, A.F. Pozharskiid, N.V. Vistorobskiid and X. Allonase
aFaculty of Chemistry, University of Wrocław, Joliot-Curie 14 st, 50-383 Wrocław, Poland
bInstitute of Physics, Polish Academy of Sciences, Al.Lotników 32/46, 02-668 Warsaw, Poland
cVan ‘t Hoff Institute of Molecular Sciences, University of Amsterdam, Nieuwe Achtergracht, 166, 1018 WV, Amsterdam, The Netherlands
dRostov State University, Zorge 7 str, 344-090 Rostov-on-Don, Russian Federation
eDepartment de Photochemie Generale, UMR CNRS No. 7525, ENSCMu, 3 rue A.Werner, 68-093 Mulhouse Cedex, France
Received 20 October 2004;
revised 21 October 2004.
Available online 30 November 2004.
Abstract
The geometric and electronic structure of 1,8-bis(dimethylamino)-4-cyano-naphthalene (DMAN-CN) and its mono-protonated cation (H+DMAN-CN) have been investigated by density functional theory (DFT) and time dependent density functional theory (TD-DFT) methods. Ground state geometry optimization leads to a significant structural asymmetry and polarity of both molecules. Vertical excitation energies and oscillator strengths calculated for the lower-lying excited singlet states of DMAN-CN are in excellent agreement with experimental absorption maxima in n-hexane. Similarly, it is found that experimentally observed solvatochromic shifts are favourably reproduced by the calculations. The calculations reveal that the S1 and S2 states of the neutral molecule and the S3 state of the cation are characterised by an asymmetric charge transfer, i.e., the two dimethylamino groups contribute unequally to the transfer of charge to the cyanonaphthalene moiety.
Fig. 1. Experimental (exp) and TD-DFT calculated (calc) absorption spectra of DMAN-CN in hexane and of H+DMAN-CN in acidified acetonitrile together with the values of their vertical excitation energies (attached table).
Fig. 2. Directions of excited state dipole moments in the ground state (S0) and in the FC excited states of DMAN-CN and H+DMAN-CN. (TD-DFT calculations).
Fig. 3. Changes of charge in DMAN-CN and H+DMAN-CN on the S0 → Si transitions (TD-DFT calculations).
Fig. 4. Experimental absorption spectrum of DMAN-CN in two different solvents.
Table 1.
Geometrical parameters for DMAN-CN and H+DMAN-CN calculated by DFT (B3LYP/6–31G**) method

Table 2.
Transition energies, oscillator strengths, components of the transition moment values and the orbital shapes of the corresponding molecular orbitals for DMAN-CN and H+DMAN-CN (TD-DFT calculations)


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