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seen in polycyclic aromatics, as the exclusive interaction, as
square-planar Ni2+ complexes 1b, 4b, 6b, and 7b do not show
similar organization to the Zn2+ complexes. TEM images of
the nickel complexes showonly ill-defined morphologies
when cast from methanol or solvent mixtures. Complexes 6
and 7 with copper or vanadyl in the place of zinc also show no
fiber assembly.
Complex 8 has bulky tert-butyl groups that should inhibit
aggregation of the zinc complexes. Indeed complex 8 does not
form a gel in methanol or in toluene, and TEM images of this
complex cast from methanol showed no fibrillar texture.
Complex 9, which is the thiol analogue to complex 4a, does
not self-assemble into fibers in methanol. In this case, the
aggregation is most likely inhibited by the bulky sulfur atoms
at the zinc center that prevent expansion of the coordination
sphere of the metal center. Additionally, the softer sulfur
atom would be expected to interact less strongly with zinc
than oxygen. These control compounds further support that
the aggregation is mediated at the metal center.
The UV/Vis spectra for films of Zn2+ complexes 1a–7a
exhibit small red-shifts and broadening relative to the
solution-phase spectra. Moreover, they are all luminescent,
emitting at 525–540 nm, red-shifted by 20 nm from the
solution phase. The similarity of the absorption and emission
spectra for solutions and films of 1a–7a indicates that a
similar aggregation mechanism is involved in both the
assembly of alkoxy- and carbohydrate-substituted complexes.
Further evidence for aggregation was obtained from
electrospray ionization mass spectra (ESI-MS) of the com-
plexes. All the spectra of the zinc complexes showed the
molecular ion, but also showed peaks corresponding to
aggregates. In fact, when the instrument was optimized for
measurements on 2a, we were able to observe singly and
doubly charged species up to nine monomers (Figure 4).
Although quantifying the individual species by ESI-MS is not
feasible, the technique is known to give a snapshot of species
present in solution. Thus, large aggregates of 2a are formed in
solution, supporting the strong tendency of these complexes
to aggregate.
Figure 4. ESI-MS spectrum of complex 2a exhibits singly (A–E) and
doubly (F–I) charged species. A: [2a+Na]+, B: [(2a)2 +Na]+, C:
[(2a)3 +Na]+, D: [(2a)4 +Na]+, E: [(2a)5 +Na]+, F: [(2a)3 +Na2]2+, G:
[(2a)5 +Na2]2+, H: [(2a)7 +Na2]2+, I: [(2a)9 +Na2]2+
.
Figure 5. Energy-minimized (PM3) calculated structure for a heptamer
of [Zn(salphen)]. a) The entire oligomer containing seven [Zn-
(salphen)] molecules connected into a 1D structure. b) An expanded
view of three [Zn(salphen)] units from the middle of the heptamer.
(Zn gray, O red, N blue, C green).
Semi-empirical (PM3) calculations were performed to
better understand the supramolecular organization in these
structures. Assuming the Zn2+ center is five-coordinate in the
fibers as observed in dimers of [Zn(salphen)]-type complexes,
an oligomer containing seven unsubstituted [Zn(salphen)]
was constructed and its energy minimized, starting from
several different conformations. Figure 5 shows an energy-
minimized structure for the 1D heptamer with five-coordinate
organization that may arise from the stacking of the salphen
moieties.
It is noteworthy that the aggregation behavior we have
observed for metal salphen complexes is distinct from that of
porphyrins.[10,18] Whereas porphyrins (and phthalocyanines)
are known to aggregate, their assembly is dominated by p–p
stacking or interactions of substituents, and the metal
dependence is generally less pronounced. As an example,
Shinkai and co-workers have observed improved gelation
properties of a copper-containing porphyrin over the analo-
gous zinc-containing porphyrin and have attributed this
improvement to the stabilization of H-aggregates.[18] The
coordination environment of salphen complexes is much
more flexible than that of porphyrin complexes, offering new
possibilities for self-assembly.
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zinc ions. Calculated Zn O and Zn N distances are in
agreement with crystallographic studies of dimers. The
polymeric backbone contains a (ZnO)n polymer as illustrated
in Figure 5, with an insulating organic sheath.
An interesting revelation from the modeling is that the
complexes assembled in the 1D structures will likely assume a
helical conformation. We have observed regions of fibers of
the zinc complexes 1a–5a that appear to have helical
structure, and it is possible this motif derives from the helical
conformation of the polymer strand. Figures 2e,f show
regions of fibers formed from compound 3a. In these
images, there are segments that appear to have helical
ꢀ 2007 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2007, 46, 7980 –7983