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Fig. 3 CO isotherms at 288 K for materials A (triangular symbols)
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´
appears to occur in a single-crystal-to-single-crystal (SCSC)
1
transformation. To confirm removal of the solvent and
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retention of porosity the crystals were exposed to I and CS
2
2
1
1,12
vapours.
The reversible change in colour with I supports
2
13
the existence of permanent pores (Fig. S4). While investigating
the desorption of I and CS from the single crystals of A it was
2
2
noted that bubbles formed at all edges of the needle-shaped
crystals (Fig. S28). This is in contrast to the pristine samples in
which no bubbles are seen when ethanol or methanol is desorbed.
Even though the crystal is undergoing a macroscopic SCSC
transformation, the material does develop a considerable amount
of cracking/defects between porous channels, allowing for the
(
f) S. A. FitzGerald, B. Burkholder, M. Friedman, J. B. Hopkins,
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14
diffusion of the I or CS perpendicular to the channel axis.
2
2
7
(a) M. O. M. Piepenbrock, G. O. Lloyd, N. Clarke and J. W. Steed,
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To further test the permanent porosity of materials A and D
gas adsorption isotherms were obtained, showing that the
materials readily adsorb CO
considerable hysteresis in the desorption isotherm of CO
Fig. 3). As the materials both undergo SCSC transformations,
2
at 288 K. Additionally, there is
2
(
2
011, 47, 5154–5156.
we are confident that the hysteresis is not caused by a structural
rearrangement of the materals or by a narrow pore window as
8 P. Zhang, Y. Y. Niu, B. L. Wu, H. Y. Zhang, C. Y. Niu and
H. W. Hou, Inorg. Chim. Acta, 2008, 361, 2609–2615.
1
5
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2
has been seen with other materials. Two CO molecules are
adsorbed per macrocycle, corresponding well with the available
void space within the material and the molecular volume of
4a
CO2. Material E was not tested due to the low yield of the
material’s synthesis; alternative methods were explored but
none were successful in producing a pure, high yield sample.
In conclusion, we have synthesised five new materials using
ligand 1. It is clear that an interplay between the inclusion of
solvent, hydrogen bonding and p–p stacking controls the supra-
molecular isomerism of this metal halide system. We have
sythesised three isostructural porous materials, two of which show
1
0 A. L. Spek, J. Appl. Crystallogr., 2003, 36, 7–13.
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´
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(
Aust. J. Chem., 2010, 63, 573–577; (c) C. E. Willans, S. French,
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1
2 K. Otsubo, Y. Wakabayashi, J. Ohara, S. Yamamoto, H. Matsuzaki,
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2
SCSC transformations, as well as CO desorption hysteresis.
2011, 10, 291–295.
Further studies on these porous materials are currently underway
to better understand the supramolecular isomerism and gas sorption
characteristics, particularly the mechanism behind the hysteresis.
G.O.L. thanks the Herchel Smith Fellowship Fund
13 S. V. Potts, L. J. Barbour, D. A. Haynes, J. M. Rawson and
G. O. Lloyd, J. Am. Chem. Soc., 2011, 133, 12948–12951.
1
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(
Cambridge) and Prof. Anthony Cheetham. J.C.T. thanks
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the European Research Council.
(
b) X. M. Liu, L. H. Xie, J. B. Lin, R. B. Lin, J. P. Zhang and
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112 Chem. Commun., 2012, 48, 2110–2112
This journal is c The Royal Society of Chemistry 2012