1
This is supported by the observation of similar H NMR and
show electrochemical behaviour compatible with four indepen-
dent redox centres and could act as four electron reservoirs.
We gratefully thank the Swiss National Science Foundation
for their support of this work.
electronic spectra for 3 and the model compound 5 (prepared
by stoichiometric mixing of 1 with methyl 4-(pyridine-4-yl)
benzoate). Despite numerous efforts, only an average mass for
3 was observed in the MALDI TOF spectrum, but exact
masses were observed for monomeric, dimeric and trimeric
fragments of 3.
Notes and references
As expected for the greater size of the square the diffusion
coefficient of 3 determined by 1H DOSY experiments at 25 1C
z Crystal data for 2: C59H78NO9.5Rh2 was collected on a IPDS II
diffractometer at 180(2) K using MoKa radiation (l = 0.71073 A).
Full-matrix, least-squares refinements on F2 using all data. Total data
128 659, unique data 8666 (Rint = 0.2164), Mr = 1159.04, cubic, space
in CDCl3 is 370 mm2
s
ꢀ1. Although the Stokes–Einstein
equation is not suitable for determination of the hydro-
dynamic radius of these complexes due to their non-spherical
shape, the order of the diffusion coefficients 1 > 2 > 3 is in
good agreement with the expected size progression.
%
group Ia3d, a = b = c = 59.616(3) A, a = b = g = 901, V =
211 879(17) A3, Z = 96, R1 [I > 2s(I)] = 0.1141, wR2 = 0.2877.
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ligands, and UV-visible titrations (Fig. S8–S10, ESIw) with a
series of pyridine bases showed two-step binding with typical
values of log10K1 of 6 and log10K2 of 3. The tetramers 2 and 3
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constants observed for the smaller tetramer 2 were slightly
greater than those for 3.
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a single quasi-reversible system (0.01 o v o 5 V sꢀ1). In the
case of monomeric complexes, we observed the one-electron
oxidation of the dirhodium(II) species: [Rh2]4+ - [Rh2]5+ +eꢀ
in the range observed for other tetracarboxylate dirhodium
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metal centres of compound 1 causes a negative shift of about
ꢀ100 mV of the potential E1/2 (Fig. S11, ESIw). This shift
reflects stabilization of the oxidized state Rh(III)–Rh(II) due to
increased electron density on the metal centres with the presence
of an additional N-donor. For 2 and 3, the cyclic voltammograms
may be interpreted in terms of four independent one-electron
oxidations showing negligible interaction. The peak observed
for 2, where the rhodium–rhodium distance is shorter, is slightly
broader than that seen for 3 which may indicate slightly greater
interaction (Fig. S12, ESIw). This affords a notable contrast with
the systems where the dirhodium units are linked by equatorial–
equatorial interactions (using terephthalate or oxalate21,22) where
significant interaction was observed.
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In conclusion, we have shown the facile one-step synthesis
of nanometre-sized squares in high yields using a new combi-
nation of reversible orthogonal interactions. Two bonds
have been used: dirhodium–carboxylate, and axial rhodium–
nitrogen binding. Heating is required for carboxylate exchange,
but when this occurs and axial coordination is possible,
the mono-substituted product is selected out of the dynamic
mixture as a result of the tetramerisation of the exchanged
product. The resulting assemblies show Lewis acidity, binding
up to four Lewis bases in the vacant axial positions, and are
potentially available for the construction, via Lewis acid–Lewis
base interactions, of more elaborate structures. They further
c
This journal is The Royal Society of Chemistry 2012
Chem. Commun., 2012, 48, 9891–9893 9893