Highly Ordered Thin Films of Octasubstituted Phthalocyanines
Paul Smolenyak,
²
Rebecca Peterson,
²
Ken Nebesny,
²
Michael To 1 rker,
‡
David F. O’Brien,*
,²
and Neal R. Armstrong*
,²
Contribution from the Department of Chemistry, UniVersity of Arizona, Tucson, Arizona 85721, and
Institute fu ¨ r Angewandte Photophysik, Technical UniVersita ¨ t Dresden, Dresden, Germany
ReceiVed May 6, 1999
Abstract: Phthalocyanines (Pc) modified at eight positions with benzyloxyethoxy groups (CuPc(OC
2
OBz)
8
and H
2
Pc(OC
2
OBz)
8
) form discotic mesophases in the bulk and self-assemble into cofacial rodlike aggregates
in monolayers. These Pc aggregates form close packed arrays which are simple to process into highly coherent
multilayer thin films. When these self-organizing molecular systems are compressed on the surface of an LB
trough, the Pc columns align parallel to the compression barriers and form a rigid bilayer film (ca. 5.6 nm
thick). Sections of these bilayer films can be mechanically removed from the trough surface with complete
retention of integrity of the remaining film. This unprecedented behavior appears to arise from the multiple
π-π interactions between adjacent Pcs, resulting in unusually strong noncovalent interactions. AFM and STM
studies of monolayer and bilayer films show that they consist of Pc columns which are coherent over distances
of 50-100 nm. Thin films consisting of up to 15 bilayers (ca. 84 nm) can be quickly built by a “mechanical
stamping” process, and small-angle X-ray scattering characterization of these film materials confirms their
unusual coherence. Large electrical and optical anisotropies are observed in multilayer films of CuPc(OC
2
-
OBz)
8
and H
2
Pc(OC
2
OBz)
8
which are comparable to those previously reported for thin film assemblies based
on side-chain-modified silicon phthalocyanine polymers.
Introduction
Molecules which form discotic mesophases with significant
long-range order and anisotropic electrical and optical properties
continue to be sought for applications in electrical or optical
logic circuits, electroluminescence devices, and electrochromic
displays, among others.
1-16
Side-chain-modified phthalocyanines
form a major class of discotic mesophase materials, and there
are multiple examples of these molecules which aggregate or
polymerize into rodlike assemblies with extremely interesting
optical and electrical properties. Tailoring conductivity, optical
band gap, luminescence energy and efficiency in thin films and
“fibers” of these materials, through changes in their composition
and molecular architecture, has been widely demonstrated.
1,6,8-10,14
Ordered organic thin films of these materials can often show
large anisotropies in these properties,
1,2,5,8-10
which might be
their most important advantage, if simple processing conditions
can sustain these anisotropies in the macroscopic material.
Highly ordered thin films have been previously created using
prepolymerized silicon phthalocyanines (PcPS), modified at
either the 4 or 8 positions on each Pc with solubilizing side
chains, forming rodlike units, each unit containing up to 100
Pcs.
1-5
These polymeric rods pack with excellent uniformity
in orientation, parallel to the vertical dipping direction used for
Langmuir-Blodgett thin film fabrication, and their large optical
and electrical anisotropies form the basis for comparison of these
properties in the materials reported here.
The disk-shaped monomeric 2,3,9,10,16,17,23,24-octakis(2-
benzyloxyethoxy)phthalocyaninato copper, and its metal free
analogue (CuPc(OC
2
OBz)
8
and H
2
Pc(OC
2
OBz)
8
(Figure 1)),
have recently been shown to exhibit a discotic mesophase in
the bulk material, and a unique degree of self-assembly into
coherent rodlike structures on the Langmuir trough.
12,13
Al-
though many different side-chain-modified Pcs and other
discotic molecules have been synthesized, few of these side
chains have been terminated with aromatic functionality, and
for those that have, the thin film properties either were not
reported or did not show the properties of the Pcs reported
here.
10,15,16
We are aware of only one other monomeric side-
chain-modified Pc (possessing chiral centers in the side chain),
8
* To whom correspondence should be addressed. E-mail: nra@
u.arizona.edu; dfobrien@u.arizona.edu.
²
University of Arizona.
‡
Technical Universita ¨t Dresden.
(1) Wegner, G. Mol. Cryst. Liq. Cryst. 1993, 235, 1.
(2) Sauer, T.; Arndt, T.; Batchelder, D. N.; Kalachev, A. A.; Wegner,
G. Thin Solid Films 1990, 187, 357
(3) Wu, J. H.; Lieser, G.; Wegner, G. AdV. Mater. 1996, 8, 151.
(4) Ries, R.; Lieser, G.; Schwiegk, S.; Wegner, G. Acta Polym. 1997,
48, 536.
(5) S ˇ ilerova ´, R.; Kalvoda, L.; Neher, D.; Ferencz, A.; Wu, J.; Wegner,
G. Chem. Mater. 1998, 10, 2284.
(6) Simon, J.; Bassoul, P. In Phthalocyanines: Properties and Applica-
tions; Lezneff, A. B. P., Ed.; VCH Publishers, Inc.: New York, 1993; Vol.
2, p 223.
(7) Toupance, T.; Bassoul, R.; Minear, L.; Simon, J. J. Phys. Chem. 1996,
100, 11704.
(8) van Nostrum, C. F.; Bosman, A. W.; Gelinck, G. H.; Schouten, P.
G.; Warman, J. M.; Kentgens, P. M.; Devillers, M. A. C.; Meijerink, A.;
Picken, S. J.; Sohling, U.; Shouten, A.-J.; Nolte, R. J. M. Chem.sEur. J.
1995, 1 (3), 171.
(9) Englekamp, H.; Meddelbeek, S.; Nolte, R. J. M. Science 1999, 284,
785.
(10) Fox, J. M.; Katz, T. J.; Van Elshocht, S.; Verbiest, T.; Kauranen,
M.; Persoons, A.; Thongpanchang, T.; Krauss, T.; Brus, L. J. Am. Chem.
Soc. 1999, 121, 3453.
(11) Cook, M. J. J. Mater. Sci.: Mater. Electron. 1994, 5, 117.
(12) Osburn, E. J.; Chau, L.-K.; Chen, S.-Y.; Collins, N.; O’Brien, D.
F.; Armstrong, N. R. Langmuir 1996, 12, 4784.
(13) Smolenyak, P. E.; Osburn, E. J.; Chen, S.-Y.; Chau, L.-K.; O’Brien,
D. F.; Armstrong, N. R. Langmuir 1997, 13, 6568.
(14) Osburn, E. J.; Schmidt, A.; Chau, L.-K.; Chen, S.-Y.; Smolenyak,
P.; Armstrong, N. R.; O’Brien, D. F. AdV. Mater. 1996, 8, 926. (15) Bryce, M. R. J. Chem. Soc., Perkin Trans. 1997, 2, 1671.
8628 J. Am. Chem. Soc. 1999, 121, 8628-8636
10.1021/ja991498b CCC: $18.00 © 1999 American Chemical Society
Published on Web 09/03/1999