ChemComm
Communication
Cadet Program’’. We thank Dr W. Bettray and C. Dittmer (IOC,
RWTH Aachen University) for MS-measurements.
Notes and references
1 (a) J. V. Barth, Annu. Rev. Phys. Chem., 2007, 58, 375–407; (b) J. A. A. W.
Elemans, L. Shengbin and S. De Feyter, Angew. Chem., Int. Ed., 2009, 48,
7298–7332.
2 D. Bonifazi, S. Mohnani and A. Llanes-Pallas, Chem. – Eur. J., 2009,
15, 7004–7025.
3 J. P. Rabe and S. Buchholz, Science, 1991, 253, 424–427.
4 (a) J. A. Theobald, N. S. Oxtoby, M. A. Phillips, N. R. Champness and
P. H. Beton, Nature, 2003, 424, 1029–1031; (b) M. Lackinger and
W. M. Heckl, Langmuir, 2009, 25, 11307–11321; (c) Y.-T. Shen, M. Li,
Y.-Y. Guo, K. Deng, Q.-D. Zeng and C. Wang, Chem. – Asian J., 2010,
5, 787–790.
Fig. 3 (a, b) An STM image and a network model of the non-porous
structure of 2 at the PO/graphite interface (1.8 ꢀ 10ꢁ5 M, Iset = 0.21 nA and
Vset = ꢁ0.31 V). White arrows in (a) indicate the directions of main
symmetry axes of underlying graphite.
5 (a) S. Stepanow, M. Lingenfelder, A. Dmitreiev, H. Spillmann,
E. Delvigne, N. Lin, X. Deng, C. Cai, J. V. Barth and K. Kern, Nat.
Mater., 2004, 3, 229–233; (b) D. Ku¨hne, F. Klappenberger, R. Decker,
U. Schlickum, H. Brune, S. Klyatskaya, M. Ruben and J. V. Barth,
J. Am. Chem. Soc., 2009, 131, 3881–3883.
6 (a) K. Tahara, S. Furukawa, H. Uji-i, T. Uchino, T. Ichikawa, J. Zhang,
W. Mamdouh, M. Sonoda, F. C. De Schryver, S. De Feyter and
Y. Tobe, J. Am. Chem. Soc., 2006, 128, 16613–16625; (b) K. Tahara,
S. Lei, J. Adisoejoso, S. De Feyter and Y. Tobe, Chem. Commun., 2010,
46, 8507–8525.
covered only with the non-porous pattern. This phase behaviour is
consistent with that of the networks formed by alkoxy-substituted
triangle p-conjugated molecules.17c,d On the other hand, only the
porous pattern was observed over a wide concentration range at the
1,2,4-trichlorobenzene (TCB)/graphite interface (see ESI,† Fig. S2)
presumably due to the stabilizing effect for porous patterns by
solvent co-adsorption.6a,18
7 (a) G. Schull, L. Douillard, C. Fiorini-Debuisschert, F. Charra,
F. Mathevet, D. Kreher and A.-J. Attias, Nano Lett., 2006, 6, 1360–1363;
´
In contrast to 1a, compound 2 formed only a non-porous pattern
even at the lowest concentration (1.8 ꢀ 10ꢁ6 M) in PO (Fig. 3a and
Fig. S3, ESI†). In this case, all three alkyl chains per molecule are
adsorbed on the surface. Unit cell parameters are a = 2.8 ꢂ 0.1 nm,
b = 3.1 ꢂ 0.2 nm, g = 60 ꢂ 41. A tentative network model is shown in
Fig. 3b. Note that the molecular core adopts the ssa-conformation.
To build a close-packed molecular network, the intermolecular
van der Waals interactions must have prevailed over the intra-
molecular hydrogen bonding interactions. The formation of the
(b) C. Arrigoni, G. Schull, D. Bleger, L. Douillard, C. Fiorini-Debuisschert,
F. Mathevet, D. Kreher, A.-J. Attias and F. Charra, J. Phys. Chem. Lett.,
2010, 1, 190–194; (c) S. Xu, Q. Zeng, J. Lu, C. Wang, L. Wan and C.-L. Bai,
Surf. Sci., 2003, 538, L451–L459.
8 K. Tahara, C. A. Johnson II, T. Fujita, M. Sonoda, F. C. De Schryver,
S. De Feyter, M. M. Haley and Y. Tobe, Langmuir, 2007, 23,
10190–10197.
¨
9 S.-S. Jester, E. Sigmund and S. Hoger, J. Am. Chem. Soc., 2011, 133,
11062–11065.
¨
10 T. Chen, G.-B. Pan, H. Wettach, M. Fritzsche, S. Hoger, L.-J. Wan,
H.-B. Yang, B. H. Northrop and P. J. Stang, J. Am. Chem. Soc., 2010,
132, 1328–1333.
non-porous network pattern from 2 supports the criterion of 11 (a) B. Baisch, D. Raffa, U. Jung, O. M. Magnussen, C. Nicolas,
J. Lacour, J. Kubitschke and R. Herges, J. Am. Chem. Soc., 2009, 131,
our molecular design.
442–443; (b) U. Jung, C. Schu¨tt, O. Filinova, J. Kubitschke, R. Herges
Similar to 1a, compounds 1b and 1c formed the porous patterns
and O. Magnussen, J. Phys. Chem. C, 2012, 116, 25943–25948.
at the PO/graphite interface (3.0 ꢀ 10ꢁ6 M, Fig. S4 and S5, ESI†), 12 (a) F. L. Scott, M. Cashman and J. Reilly, J. Am. Chem. Soc., 1952,
74, 5802; (b) I. M. Mu¨ller and R. Robson, Angew. Chem., Int. Ed.,
revealing that the counter anion does not influence the self-
assembling behaviour of these molecules. In all cases, however,
¨
2000, 39, 4357–4359; (c) I. M. Mu¨ller and D. Moller, Eur. J. Inorg.
Chem., 2005, 257–263.
the counter anions were not visualised in the image, presumably 13 In crystalline state, H6L chloride and tris(5-bromo-2-hydroxybenzylidene)-
triaminoguanidinium chloride adopted saa- and aaa-conformation,
respectively, because of interactions between the chloride anion and
hydroxy groups. See ref. 12b and c.
because of their dynamic behaviour in the liquid phase or low
tunneling efficiency.19
´
In summary, we have shown that tris-(2-hydroxy-benzylidene)tri- 14 R. Lazzaroni, A. Calderone, G. Lambin, J. P. Rabe and J. L. Bredas,
Synth. Met., 1991, 41, 525–528.
aminoguanidinium salts having six alkyl chains with proper spacing
served as new molecular building blocks for the formation of porous
15 Orbital distributions of HOMO and HOMO ꢁ 1 of 1+ are located at
the peripheral three aryl units (see ESI,† Fig. S6).
networks by van der Waals interactions at the liquid/graphite inter- 16 Y. Yang and C. Wang, Curr. Opin. Colloid Interface Sci., 2009, 14,
135–147.
faces. The counter anions did not influence the self-assembling
behaviour, forming the identical honeycomb networks. Given the
17 (a) L. Kampschulte, T. L. Werblowsky, R. S. K. Kishore, M. Schmittel,
W. M. Heckl and M. Lackinger, J. Am. Chem. Soc., 2008, 130, 8502–8507;
co-adsorption capability for nonpolar guest molecules at the pores of
the honeycomb networks,2,6,7 the present molecular networks would
serve as templates for complex 2D patterns formed by multiple
interactions. Additionally, since H6L salts are known to form transi-
tion metal complexes,12b,20 construction of 2D metal arrays which may
serve as tailor made catalysts would become possible.
(b) C.-A. Palma, J. Bjork, M. Bonini, M. S. Dyer, A. Llanes-Pallas,
`
D. Bonifazi, M. Persson and P. Samorı, J. Am. Chem. Soc., 2009, 131,
13062–13071; (c) S. Lei, K. Tahara, F. C. De Schryver, M. Van der Auweraer,
Y. Tobe and S. De Feyter, Angew. Chem., Int. Ed., 2008, 47, 2964–2968;
(d) A. Bellec, C. Arrigoni, G. Schull, L. Douillard and C. Fiorini-
Debuisschert, J. Chem. Phys., 2011, 134, 124702.
18 M. O. Blunt, J. Adisoejoso, K. Tahara, K. Katayama, M. Van der Auweraer,
Y. Tobe and S. De Feyer, J. Am. Chem. Soc., 2013, 135, 12068–12075.
This work was supported by the JSPS Japanese-German Graduate 19 (a) S. Takahashi, A. Aramata, M. Nakamura, K. Hasebe, M. Taniguchi,
S. Taguchi and A. Yamagishi, Surf. Sci., 2002, 512, 37–47; (b) Y. Xiao,
G.-B. Pan and W. Freyland, Chem. Phys. Lett., 2009, 481, 91–93.
Externship, the Deutsche Forschungsgemeinschaft through the
International Research Training Group SeleCa (IGRK 1628), and
Programs Leading Graduate Schools: ‘‘Interactive Material Science
´
¨
20 I. M. Oppel (nee Mu¨ller) and K. Focker, Angew. Chem., Int. Ed., 2008,
47, 402–405.
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