C O M M U N I C A T I O N S
are sufficient to vary the solid-state structure. Surprinsingly, this result
is independent of the Si surface chemistry.
In conclusion, the crystalline assemblies of 1 and 2, fabricated by
PVD, exhibit controllable film morphologies. In particular, the surface
morphology of 2-based assemblies can be varied from elongated
features, cone-shaped grains, and interconnected islands to relatively
large grains. Crystal growth morphology and molecular-based thin film
formation guided by monolayer-based interfaces is of major interest.9
On the other hand, the corresponding film microstructures are
independent of the substrate surface chemistry. This is very surprising
for an organic thin film.2 The molecular packing of 1-based assemblies
is identical to solution grown crystals, whereas the thin films of
compound 2 consist of a different polycrystalline structure. Apparently,
introduction of an N-oxide moiety results in a looser crystal packing,
which varies upon interaction with the substrate surface. However, in
both cases, film XRD experiments demonstrate that the solid-state
structure is independent of the substrate surface chemical functional-
ization. Since PVD is an established method for forming high-quality
molecular-based electronic materials,10 we believe that halogen-bonded
thin films may evolve into high-quality functional materials necessary
for the development of new organic optoelectronic devices.2,11
Figure 2. AFM images of 1- and 2-based films. (a, b) Compound 1 deposited
on bare silicon (10 and 100 nm, respectively); (c, d) compound 2 deposited on
bare silicon (10 nm) and on silicon substrates functionalized with a 3-based
monolayer (10 nm), respectively.
Acknowledgment. This research was supported by Minerva and
the U.S.-Israel Binational Science Foundation. M.E.vd.B. is the
incumbent of the Dewey David Stone and Harry Levine Career
Development Chair.
Supporting Information Available: Experimental details for the
formation of compound 2, PVD experiments with compounds 1 and 2.
This material is available free of charge via the Internet at http://
pubs.acs.org.
References
(1) (a) Desiraju, G. R. Angew. Chem., Int. Ed. 2007, 46, 8342. (b) Cragg, J. P.
A Practical Guide to Supramolecular Chemistry; John Wiley & Sons, Ltd.:
New York, 2005. (c) Jean-Marie, L. Supramolecular Chemistry: Concepts
and PerspectiVes; Wiley-VCH: Weinheim, Germany, 1995. (d) Schneider,
H. J. Angew. Chem., Int. Ed. Engl. 1991, 30, 1417.
(2) (a) Kim, C.; Facchetti, A.; Marks, T. J. Science 2007, 318, 76. (b) Yoon,
M.-H.; Facchetti, A.; Marks, T. J. Proc. Natl. Acad. Sci. U.S.A. 2005, 102,
4678.
(3) (a) Metrangolo, P.; Resnati, G. Halogen Bonding: Fundamentals and
Applications; Springer: Berlin, 2007; Vol. 126. (b) Metrangolo, P.;
Neukirch, H.; Pilati, T.; Resnati, G. Acc. Chem. Res. 2005, 38, 386.
(4) Auffinger, P.; Hays, F. A.; Westhof, E.; Ho, P. S. Proc. Natl. Acad. Sci.
U.S.A. 2004, 101, 16789.
Figure 3. Experimental and simulated X-ray diffraction patterns of compounds
1 and 2. (a) Compound 1 on a silicon substrate modified with a 3-based
monolayer (10 nm, blue) and on bare silicon (100 nm, black). (b) Compound
2 on a silicon substrate modified with a 3-based monolayer (10 nm, blue) and
on bare silicon (100 nm, black). (c, d) Simulated XRD powder patterns with
selected reflections labeled for compounds 1 and 2, respectively.
XRD measurements of the XB films show strong diffraction
patterns, demonstrating the film’s polycrystalline nature (Figures 3,
S3, and S4). These films are far more textured than PVD grown films
based on hydrogen bonding.2b These experiments were carried out in
two reflection modes for 100 nm thick films: (i) specular diffraction,
θ-2θ scans, which probe the crystallographic planes parallel to the
plane of the substrate and (ii) asymmetric, 2θ, scans (incident angle
2°) that provide information independently of the crystallite preferred
orientation. The 10 nm thick films were scanned in the 2θ mode. The
XRD patterns indicate that the assemblies grown on different interfaces
have similar crystalline phases—no preferred orientation of crystallites
was observed. The XRD signals of the 1-based assemblies grown on
bare silicon and those grown on 3-based monolayers on silicon
substrates match well with the single-crystal lattice. The intensity of
the set of peaks increases with increasing film thickness (from 10 to
100 nm, Figure 3), indicating that the structural order remains
unchanged during the film growth process. The simulated powder
pattern was used to assign the observed reflections (Figure 3c,d). The
microstructures of the 1-based films and the single crystal grown from
solution are identical.8 In contrast, the polycrystalline assemblies of
compound 2 are different from the single-crystal structure. Several
reflections are significantly shifted in comparison with the simulated
powder pattern, demonstrating that 2-substrate surface interactions
(5) (a) Vartanian, M.; Lucassen, A. C. B.; Shimon, L. J. W.; van der Boom,
M. E. Cryst. Growth Des. 2008, 8, 786. (b) Metrangolo, P.; Meyer, F.;
Pilati, T.; Proserpio, D. M.; Resnati, G. Chem.—Eur. J. 2007, 13, 5765.
(c) Politzer, P.; Lane, P.; Concha, M. C.; Ma, Y. G.; Murray, J. S. J. Mol.
Model. 2007, 13, 305–311. (d) Glaser, R.; Knotts, N.; Yu, P.; Li, L. H.;
Chandrasekhar, M.; Martin, C.; Barnes, C. L. Dalton Trans. 2006, 2891.
(e) Reddy, C. M.; Kirchner, M. T.; Gundakaram, R. C.; Padmanabhan,
K. A.; Desiraju, G. R. Chem.—Eur. J. 2006, 12, 2222. (f) Caronna, T.;
Liantonio, R.; Logothetis, T. A.; Metrangolo, P.; Pilati, T.; Resnati, G.
J. Am. Chem. Soc. 2004, 126, 4500.
(6) Wash, P. L.; Ma, S.; Obst, U.; Rebek, J. J. J. Am. Chem. Soc. 1999, 121,
7973.
(7) Zaman, B.; Udachin, K. A.; Ripmeester, J. A. Cryst. Growth Des. 2004, 4,
585.
(8) Lucassen, A. C. B.; Zubkov, T.; Shimon, L. J. W.; van der Boom, M. E.
CrystEngComm 2007, 9, 538.
(9) (a) Altman, M.; Zenkina, O.; Evmenenko, G.; Dutta, P.; van der Boom,
M. E. J. Am. Chem. Soc. 2008, 130, 5040. (b) Aizenberg, J.; Black, A. J.;
Whitesides, G. M. Nature 1999, 398, 495. (c) Mann, S.; Heywood, B. R.;
Rajam, S.; Birchall, J. D. Nature 1988, 334, 692.
(10) (a) Sun, Y.; Tan, L.; Jiang, S.; Qian, H.; Wang, Z.; Yan, D.; Di, C.; Wang,
Y.; Wu, W.; Yu, G.; Yan, S.; Wang, C.; Hu, W.; Liu, Y.; Zhu, D. J. Am.
Chem. Soc. 2007, 129, 1882. (b) Yoshimura, T.; Ito, S.; Nakayama, T.;
Matsumoto, K. Appl. Phys. Lett. 2007, 91, 033103. (c) Tang, Q.; Li, H.;
Liu, Y.; Hu, W. J. Am. Chem. Soc. 2006, 128, 14634. (d) Yoshimura, T.;
Tatsuura, S.; Sotoyama, W.; Matsuura, A.; Hayano, T. Appl. Phys. Lett.
1992, 60, 268. (e) Yoshimura, T.; Tatsuura, S.; Sotoyama, W. Appl. Phys.
Lett. 1991, 59, 482.
(11) (a) Burtman, V.; Ofir, Y.; Yitzchaik, S. Langmuir 2001, 17, 2137. (b) Shi,
Y.; Zhang, C.; Zhang, H.; Bechtel, J. H.; Dalton, L. R.; Robinson, B. H.;
Steier, W. H. Science 2000, 288, 119. (c) Burtman, V.; Zelichenok, A.;
Yitzchaik, S. Angew. Chem., Int. Ed. 1999, 38, 2041.
JA8029784
9
J. AM. CHEM. SOC. VOL. 130, NO. 26, 2008 8163