exocyclic P–Ag–P coordination by the third triphosphine
arm. This unit is based on the ‘silver-diphos’ dinuclear ring
which occurs commonly with diphosphines.5d The DLS results
from pH 6.0–3.5 indicate that the intermediate is relatively
small (DH = 1.5 nm Æ 0.3 nm) (Fig. 3d). The smallest possible
cyclic oligomer based on this repeat unit would be for n = 2,
i.e. an Ag6L4hexasilver ring (Fig. 2b). Interestingly, this ring
would be a cyclic isomer of the adamantoid cage. It suggests
that the polymer itself may also be based on this basic repeat
unit, and in fact, this type of topology has been previously seen
with a related triphosphine in the crystalline state.6 On further
decreasing the pH (2 and 1.5), the intermediate disappeared
and the adamantoid cage became the sole species present.
A
coherent overall scheme for the {(AgOTf)3L2}
system which accounts for the NMR and DLS data is shown
in Fig. 2b. The discrete cage forms when hydrophobic
interactions are either absent (organic solvents) or are
overcome by head-group protonation (low pH) whereas a
large globular coordination polymer based on a different
connectivity forms when hydrophobic interactions are
present (in pure water). This responsiveness clearly parallels
that of true micelles as illustrated by the behaviour of free L.
Interestingly, this study shows that micellar imitation can also
give rise to unexpected types of assembly such as the
intermediate seen here.
Fig. 4 Molecular model of the pseudo-micellar cage complex
[Ag6L4(OTf)4]2+ (white spheres = Ag, yellow = P and S, green = F,
phenylene groups = cyan, piperazine groups = blue).
In summary, we demonstrate the extension of micellar
imitation by simple metal complexes to much larger
structures. As such it is shown to be a novel approach to
controlling coordination-based self-assembly.
groups (see ESIw for details). It exhibits a pseudo-micellar
structure, i.e. the six central metal ions are surrounded by a
hydrophobic core region, which is in turn surrounded by a
hydrophilic shell of 24 diamine head groups. Importantly, the
model reveals that the hydrophobic core would still remain
partially exposed to the solvent. Consistent with our previous
study,3 this helps to explain why the cage rearranges into an
alternative, polymeric structure in non-acidified water, i.e. to
provide better shielding of the hydrophobic parts of the ligands
from the solvent.
We thank EPSRC (GR/S73860/01) for partial support of
this work.
Notes and references
1 (a) M. Fujita, Chem. Soc. Rev., 1998, 27, 417; (b) R. W. Saalfrank
and B. Demleitner, Transition Metals in Supramolecular Chemistry,
in Perspectives in Supramolecular Chemistry, ed. J. P. Sauvage,
Wiley-VCH, Weinheim, 1999, vol. 5, pp. 1–51; (c) D. L. Caulder
and K. N. Raymond, Acc. Chem. Res., 1999, 32, 975;
(d) S. Leininger, B. Olenyuk and P. J. Stang, Chem. Rev., 2000,
100, 853; (e) G. F. Swiegers and T. J. Malefetse, Coord. Chem. Rev.,
2002, 225, 91; (f) S. L. James, Chem. Soc. Rev., 2009, 38, 1744.
2 (a) R. J. Stokes and D. F. Evans, Fundamentals of Interfacial
Engineering, Wiley-VCH, Inc., 1996, ch. 5; (b) J. H. Fendler,
Membrane Mimetic Chemistry, Wiley-Interscience, 1982.
A further and unexpected point of interest was that an
intermediate was observed by both 31P NMR and DLS
during the break up of the polymer when titrated with acid.
The 31P NMR spectrum at pH 3.5 (which corresponds to
addition of one H+ per piperazine group) shows a main pair
of doublets due to the adamantoid cage (marked *, Fig. 3b).
3 N. Giri and S. L. James, Chem. Commun., 2011, DOI: 10.1039/
c0cc00648c.
There are two further pairs of doublets in an approximate 2 : 1
1
intensity ratio labelled PA (d = À5.2 ppm, J(109AgÀ31P)
=
4 K. G. Furton and A. Norelus, J. Chem. Educ., 1993, 70, 254.
5 (a) S. L. James, D. M. P. Mingos, A. J. P. White and D. J. Williams,
Chem. Commun., 1998, 2323; (b) P. W. Miller, M. Nieuwenhuyzen,
X. Xu and S. L. James, Chem. Commun., 2002, 2008; (c) X. Xu,
E. J. MacLean, S. J. Teat, M. Nieuwenhuyzen, M. Chambers and
S. L. James, Chem. Commun., 2002, 78; (d) P. W. Miller,
M. Nieuwenhuyzen, J. P. H. Charmant and S. L. James, Inorg.
Chem., 2008, 47, 8367; (e) S. L. James, E. Lozano and
M. Nieuwenhuyzen, Chem. Commun., 2000, 617.
6 This is an indicative value estimated from the unit cell volume in the
coordination polymer [Ag3{1,3,5-(PPh2)3C6H3}(OTf)3] where Z = 1
(Cambridge Crystallographic Database code MIJXUZ), see
X. L. Xu, M. Nieuwenhuyzen, J. Y. Zhang and S. L. James,
J. Inorg. Organomet. Polym. Mater., 2005, 15, 431.
592 Hz) and PB (partially coincident with the signals for the
1
cage), with J(109AgÀ31P) estimated as 590 Hz. The signals of
this intermediate cannot be unambiguously assigned.
However, PA and PB appear to constitute a single spin
system since there is a smaller coupling of ca. 6 Hz, close to
the limit of resolution but which is just resolved for PA, which
can be ascribed to a four-bond PA–PB through-backbone
coupling. The approximate 2 : 1 intensity ratio between PA
and PB is also consistent with an AB2 spin system (with regard
to only the 31P nuclei). A structural unit consistent with this
spin system, the magnitudes of the P–Ag couplings (indicating
AgP2 centres)7 and the 3 : 2 Ag : L stoichiometry is shown in
Fig. 3c. It has 10-membered {Ag}2 rings connected by
7 J. G. Verkade and L. D. Quin, Methods in Stereochemical Analysis,
Phosphorus-31 NMR spectroscopy in Stereochemical Analysis,
VCH Publishers Inc., Deerfield Beach, FL, 1987, vol. 8.
c
1460 Chem. Commun., 2011, 47, 1458–1460
This journal is The Royal Society of Chemistry 2011