INTERACTIONS IN CRYSTALS .89. DONOR ACCEP TOR COMPLEXES OF ALKYL AND AMINOBENZENES, ANTHRACENE OR PYRENE AND 1,3,5-CYANO/NITRO-BENZENES - CRYSTALLIZATION, STRUCTURES AND ELECTRONIC-SPECTRA/
H. Bock et al., INTERACTIONS IN CRYSTALS .89. DONOR ACCEP TOR COMPLEXES OF ALKYL AND AMINOBENZENES, ANTHRACENE OR PYRENE AND 1,3,5-CYANO/NITRO-BENZENES - CRYSTALLIZATION, STRUCTURES AND ELECTRONIC-SPECTRA/, Zeitschrift fur Naturforschung. B, A journal of chemical sciences, 51(11), 1996, pp. 1538-1554
The following mixed-stack donor/acceptor complexes {D ... A}(infinity)
have been crystallized and their structures determined: {hexamethylbe
nzene ... 3,5-dicyano-1-nitrobenzene}(infinity), {hexamethylbenzene ..
. 3,5-dinitro-1-cyanobenzene}(infinity), {pyrene ... 3,5-dinitro-1-cya
nobenzene}(infinity), {anthracene ...(3,5-dinitro-1-cyanobenzene)(2)}(
infinity), {N,N-dimethylanilin ... 3,5-dinitro-1-cyanobenzene}(infinit
y) and {1,3-phenylenediamine ... 3,5-dinitro-1-cyanobenzene}(infinity)
. Their lattice packing consists of parallel layers, which contain eit
her donors adn acceptors as for hexamethylbenzene and pyrene or compos
ite ones as in the 1:2 complex of anthracene with each one of the acce
ptors above and below its peripheral rings. The isostructural hexameth
ylbenzene complexes exhibit almost identical packing coefficients as w
ell as a hexagonal coplanar arrangement of the C-6(CH3)(6) donors. Wea
k intermolecular van der Waals interactions are also observed between
antiparallel cyano substituents. The interplanar pi distances range be
tween 334 and 353 pm, i.e. around 340 pm of two van der Waals pi radii
. In none of the complexes, however, significant structural changes in
either the donor or the acceptor components due to the complex format
ion are observed. In both the crystals as well as in solution, the don
or/acceptor complexes exhibit colours between yellow and red; their lo
ng-wavelength charge transfer absorption maxima, therefore, correspond
to a lowering in excitation energy of only up to 1 eV relative to tha
t of the components. The different charge transfer in the ground and t
he CT excited states is also discussed referring to other data such as
vertical first ionization energies of interplanar distances {D ... A}
, as well as to results from semiempirical calculations based on the c
rystal structure data determined adn including approximate configurati
on interaction.