E. Seikel et al. / Inorganica Chimica Acta 374 (2011) 119–126
125
pounds have been characterized by NMR and UV–Vis spectroscopy
and they show enhanced thermal stability compared to n-alkyl
substituted Pc’s. Therefore the benefits of solubility and thermal
robustness are combined in compounds 1, 2b and 3b. The molecu-
lar structure of 1 reveals that the titanyl group creates a dome over
the macrocycle. As a consequence two sets of endo and exo methyl
groups are observed in 1H and 13C NMR spectra. Face-to-face dimer
formation is hindered by this bulky ligand. To the best of our
knowledge, this is the first crystal structure reported for a soluble
non-aggregated titanyl phthalocyanine. Our next goals are investi-
gations of collective optophysical properties and of the reactivity of
these new titanyl phthalocyanines. Special focus will lie on physi-
cal vapour deposition experiments and the physical investigation
of ordered mono- and multilayers of 1.
Appendix A. Supplementary material
Fig. 7. Molecular packing of 1, view along the Ti@O bond. Ligand periphery, H
atoms and molecules of chloroform are omitted for clarity.
Selected NMR and UV–Vis spectra are given in the supporting
information. Supplementary data associated with this article can
atoms. The distance between the titanium atom and the plane de-
fined by N1, N10, N3 and N30 is 0.748(3) Å. The macrocycle slightly
deviates from planarity, adapting a ‘saddle’ conformation [19]. In
[PcTiO], a ‘saucer’ conformation is present [15]. The difference in
the chemical environment of the endo and exo methyl groups is
represented by the different distances O1–C18 (8.67(1) Å) and
O1–C17 (9.03(0) Å). The bond distances Ti1–O1 (1.619(8) Å), Ti1–
N1 (2.139(9) Å) and Ti1–N3 (2.112(1) Å) as well as the angles
N1–Ti1–O1 (111.0(5)°) and N3–Ti1–O1 (112.3(5)°) are comparable
to those reported for the unsubstituted complex [PcTiO] [15]. Se-
lected bond distances and angles are summarized in Table 2.
The lattice structure of 1 is shown in Figs. 6 and 7. Three disor-
dered molecules of chloroform are located between the macrocycle
layers and are omitted for clarity. The orientation of the titanyl
moiety is disordered due to the steric bulk induced by the periph-
eral methyl groups, since no disorder occurs in unsubstituted
[PcTiO]. The macrocycles are oriented essentially coplanar in a
slipped-stacked manner [19]. The distances between the titanium
atoms of two neighbouring macrocyles are 12.471(4) Å and
12.468(4) Å, respectively. This distance is significantly longer than
in unsubstituted [PcTiO] (daverage = 6.701 and 9.720 Å for the two
polymorphs) [15]. The distances between the ligand layers (plane
through N1, N10, N3 and N30) are 9.800 and 9.652 Å and lie be-
tween the values for the two polymorphs reported by Hiller et al.
(daverage = 4.879 and 12.281 Å, respectively). The aromatic systems
of neighbouring macrocycles overlap partially (Fig. 7), but the
overlapping area is much smaller than in the crystal phases 1
and 2 of [PcTiO] [13]. This should be a crucial factor regarding
the semiconducting and photophysical properties of 1. It is known
from fluorescence spectroscopy that the excited state lifetime of
phthalocyanines decreases with an increase of aggregation be-
tween the molecules, as non-radiative excited state quenching oc-
curs [39–43]. This has hampered the application of Pc’s in dye
sensitized solar cells [39,40]. The structure of 1 shows that by
introduction of the annellated cyclohexene moiety the aggregation
in solid state could be minimized, and hence less intermolecular
fluorescence quenching can be expected.
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Novel titanyl phthalocyanines 1, 2a, 2b, 3a and 3b have been
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