C O M M U N I C A T I O N S
smoothly from motif II to motif III without introducing defects,
and (2) the structural similarity of tectons 3 and 4, which allows
them to be interchanged without completely interrupting the growth
of an extensively hydrogen-bonded network. Further experiments
revealed that 2D crystallization of tecton 4 can be thwarted by the
addition of less than 15% of compound 3.
Our work demonstrates that a deep understanding of 2D and 3D
molecular assembly can be attained by an integrated approach using
the tools of X-ray diffraction, STM, computation, and molecular
synthesis. In particular, our results provide new guidelines for
designing 2D and 3D molecular glasses,16 as well as detailed models
for their structures and the phenomenon of polyamorphism.
Furthermore, our work confirms that molecules with well-defined
shapes and multiple sites that engage in strong directional interac-
tions are a consistently productive source of new materials with
properties not previously observed.
Acknowledgment. We are grateful to the Natural Sciences and
Engineering Research Council of Canada, the Canadian Institutes
of Health Research, the Ministe`re de l’EÄ ducation du Que´bec, the
Canada Foundation for Innovation, and the Canada Research Chairs
Program for financial support.
Figure 3. (a) STM image of the assembly produced by the adsorption of
tecton 3 on HOPG (deposition from heptanoic acid, with Vbias ) -1.5 V
and Iset ) 50 pA). (b and c) Higher-resolution images of the areas in Figure
3a highlighted in green and blue, respectively, with superimposed models.
These images show regions of local order according to motifs II (parallel
network) and III (Kagome´ network), as well as the smooth transition
between them.
According to a recent study of the 2D crystallization of tectons
on HOPG, directional interactions between adsorbates can be more
important than diffuse interactions with the surface in determining
the ultimate structure and its orientation.13 Extensive hydrogen
bonding of tectons 2-4 should make interadsorbate interactions
particularly important. Indeed, the tetraethyl esters of tectons 3-4
produced distinctly different nanopatterns on HOPG. Moreover,
networks derived from tectons 2 and 4 did not show a preferred
orientation with respect to the underlying surface.
Supporting Information Available: Syntheses of compounds 3-4,
detailed description of the calculations, and additional STM images.
This material is available free of charge via the Internet at http://
pubs.acs.org.
References
(1) Wuest, J. D. Chem. Commun. 2005, 5830-5837. Hosseini, M. W. Acc.
Chem. Res. 2005, 38, 313-323.
DFT/B3LYP calculations have suggested that the contrasting
preferences of tectons 2 and 4 for networks II and III result in
part from subtle differences in hydrogen bonding.10,14 For short
tecton 2, the cyclic tetramer that generates parallel network II is
estimated to be 0.95 kcal/mol more stable per hydrogen bond than
the Kagome´ alternative III; in contrast, elongated analogue 4 is
estimated to favor the Kagome´ structure by 0.42 kcal/mol.
For intermediate compound 3, however, the two possible
networks are predicted to have virtually identical energies. Adsorp-
tion of tecton 3 on HOPG generated a nanopattern strikingly unlike
those produced by analogues 2 and 4 (Figure 3a). In the new pattern,
individual molecules were again well resolved, presumably in part
because they are held in place by multiple hydrogen bonds. Motifs
II and III (Figure 1) can be clearly discerned in small areas of
local order (Figure 3b,c); however, large-scale periodicity apparently
cannot be attained, possibly because the two motifs are closely
matched in energy and can merge smoothly. Nevertheless, the
assembly shows a high degree of order, and most molecules have
specific orientations relative to their neighbors, resulting from the
formation of hydrogen bonds according to motifs II and III. We
suggest that Figure 3a provides an atomically resolved image of
the organization of a 2D molecular glass. It is possible to imagine
an alternative aperiodic arrangement in which the molecular
components do not have preferred orientations with respect to their
immediate neighbors. In this way, Figure 3a illustrates in 2D the
possibility of polyamorphism, in which a single molecular material
can exist as distinctly different amorphous phases.15
(2) Simard, M.; Su, D.; Wuest, J. D. J. Am. Chem. Soc. 1991, 113, 4696-
4698.
(3) For recent examples, see: (a) Maly, K. E.; Gagnon, E.; Maris, T.; Wuest,
J. D. J. Am. Chem. Soc. 2007, 129, 4306-4322. (b) Roques, N.; Maspoch,
D.; Wurst, K.; Ruiz-Molina, D.; Rovira, C.; Veciana, J. Chem. Eur. J.
2006, 12, 9238-9253. (c) Lena, S.; Brancolini, G.; Gottarelli, G.; Mariani,
P.; Masiero, S.; Venturini, A.; Palermo, V.; Pandoli, O.; Pieraccini, S.;
Samor`ı, P.; Spada, G. P. Chem. Eur. J. 2007, 13, 3757-3764. (d) Perdiga˜o,
L. M. A.; Champness, N. R.; Beton, P. H. Chem. Commun. 2006, 538-
540. (e) Nath, K. G.; Ivasenko, O.; Miwa, J. A.; Dang, H.; Wuest, J. D.;
Nanci, A.; Perepichka, D. F.; Rosei, F. J. Am. Chem. Soc. 2006, 128,
4212-4213. (f) Sokolov, A. N.; Frisˇcˇic´, T.; MacGillivray, L. R. J. Am.
Chem. Soc. 2006, 128, 2806-2807. (g) Sudik, A. C.; Coˆte´, A. P.; Wong-
Foy, A. G.; O’Keeffe, M.; Yaghi, O. M. Angew. Chem., Int. Ed. 2006,
45, 2529-2533.
(4) Herbstein, F. H. In ComprehensiVe Supramolecular Chemistry; Atwood,
J. L., Davies, J. E. D., MacNicol, D. D., Vo¨gtle, F., Eds.; Pergamon:
Oxford, U.K., 1996; Vol. 6, pp 61-83.
(5) Lackinger, M.; Griessl, S.; Heckl, W. M.; Hietschold, M.; Flynn, G. W.
Langmuir 2005, 21, 4984-4988.
(6) (a) Kampschulte, L.; Lackinger, M.; Maier, A.-K.; Kishore, R. S. K.;
Griessl, S.; Schmittel, M.; Heckl, W. M. J. Phys. Chem. B 2006, 110,
10829-10836. (b) Ruben, M.; Payer, D.; Landa, A.; Comisso, A.;
Gattinoni, C.; Lin, N.; Collin, J.-P.; Sauvage, J.-P.; De Vita, A.; Kern, K.
J. Am. Chem. Soc. 2006, 128, 15644-15651.
(7) Trimesic acid (1) can form other networks based on alternative modes of
association of -COOH groups, such as cyclic trimers.5
(8) For a previous observation of a 2D Kagome´, network, see: Tahara, K.;
Furukawa, S.; Uji-i, H.; Uchino, T.; Ichikawa, T.; Zhang, J.; Mamdouh,
W.; Sonoda, M.; De Schryver, F. C.; De Feyter, S.; Tobe, Y. J. Am. Chem.
Soc. 2006, 128, 16613-16625.
(9) Coles, S. J.; Holmes, R.; Hursthouse, M. B.; Price, D. J. Acta Crystallogr.
2002, E58, o626-o628.
(10) See the Supporting Information for details.
(11) Aujard, I.; Baltaze, J.-P.; Baudin, J.-B.; Cogne´, E.; Ferrage, F.; Jullien,
L.; Perez, E.; Pre´vost, V.; Qian, L. M.; Ruel, O. J. Am. Chem. Soc. 2001,
123, 8177-8188.
(12) Alternatively, adsorption may induce planarization, and the varying contrast
may arise from a moire´ pattern.
The frustrated crystallization of tecton 3 suggested that the 2D
cocrystallization of mixtures of compounds 2-4 would also prove
to be difficult. Deposition of a 1:1 mixture of tectons 3 and 4 on
HOPG under the standard conditions failed to yield large periodic
domains, as determined by STM.10 Again, the images showed
clearly resolved molecules oriented locally according to motifs II
and III; however, sustained growth of single crystalline phases was
not observed. We attribute the frustrated crystallization to a
combination of two synergistic effects: (1) the feasibility of moving
(13) Dang, H.; Maris, T.; Yi, J.-H.; Rosei, F.; Nanci, A.; Wuest, J. D. Langmuir,
in press.
(14) For a recent example of the use of DFT calculations to study hydrogen-
bonded networks, see: Trolliet, C.; Poulet, G.; Tuel, A.; Wuest, J. D.;
Sautet, P. J. Am. Chem. Soc. 2007, 129, 3621-3626.
(15) Poole, P. H.; Grande, T.; Sciortino, F.; Stanley, H. E.; Angell, C. A. Comp.
Mater. Sci. 1995, 4, 373-382.
(16) For a related study, see: Lebel, O.; Maris, T.; Perron, M.-EÅ .; Demers, E.;
Wuest, J. D. J. Am. Chem. Soc. 2006, 128, 10372-10373.
JA0742535
9
J. AM. CHEM. SOC. VOL. 129, NO. 45, 2007 13775