Inorg. Chem. 2010, 49, 6787–6789 6787
DOI: 10.1021/ic100785r
Metal-Interrupted Perylene Diimide: Toward a New Class of Tunable n-Type
Inorganic-Organic Hybrid Semiconductors
Kate R. Edelman and Bradley J. Holliday*
Department of Chemistry and Biochemistry and Center for Electrochemistry, The University of Texas at Austin,
1 University Station, A5300, Austin, Texas 78712-0165
Received April 27, 2010
In organic thin-film transistors (OTFTs), organic electron-transport
materials (n-type semiconductors) are well behind the advances in
development of hole-transport materials (p-type semiconductors).
Currently, one class of organic n-type semiconductor materials that
is widely utilized is N,N0-dialkyl-3,4,9,10-perylenetetracarboxylic
diimide (PTCDI-R) derivatives with high electron affinities (EAs),
such as N,N0-dioctyl-3,4,9,10-perylenetetracarboxylic diimide with
a reported EA as high as 4.4 eV. The PTCDI-R derivatives have
been manipulated by adding substituents on the perylene moiety or
at the amine position to afford more stable compounds and higher
EAs. On the basis of these materials, we have developed metal-
containing perylenediimide analogues, placing a salpen ligand for
metal ion chelation between two n-isobutylnaphthalimides. We
demonstrate here that the electronic properties of this class of
materials can be systematically tuned in a divergent manner by
simply changing the metal center. The synthesis, characterization,
electrochemistry, and band-gap analysis are discussed herein.
difficult to create robust OTFTs, which perform well when
doped. In addition, improving electron injection and trans-
port in organic devices requires materials with high electron
affinities (EAs).5,6 Specifically, organic transistors require
EA values of about 4.0 eV or higher to create ohmic contacts
to aluminum electrodes and even higher for gold elec-
trodes.7,8 Finally, tuning of the EA of organic semiconduc-
tors usually involves the addition of electron-withdrawing
substituents (i.e., -CN or F), and this often requires lengthy
tedious synthetic procedures.
To date, examples of organic n-type materials with high
EAs include hexadecafluorocopper phthalocyanine (F16CuPc)
and N,N0-dialkyl-3,4,9,10-perylenetetracarboxylic diimide de-
rivatives. The EA value for F16CuPc is 3.4 eV, and that of
N,N0-dioctylperylene-3,4,9,10-tetracarboxylic diimide (PTCDI-
C8) is 4.4 eV.9,10 The perylene diimides are of particular interest
not only because of high EAs but also because of the fact
that the electronic properties can be tuned in a rational way
through synthetic manipulations of the substituents around
the aromatic core.11,12 Herein, we describe a new class of
materials with the potential for use as n-type organic electro-
nics whereby a perylene diimide aromatic structure is inter-
rupted by a Schiff-base metal complex (Scheme 1). This
strategy has been developed, in part, to take advantage of
the ability to tune the electronic properties of these complexes
by simply changing the metal center.
Organic semiconductors were identified as early as 1940,
but low charge mobilities hindered the development of
practical applications of these materials. It was not until
the late 1980s when work on organic thin-film transistors
(OTFTs) reignited research on both polymer- and small-
molecule-based organic electronics.1-3 Organic materials are
advantageous over the inorganic counterparts because of
their ability to create flexible devices that can be produced on
a large scale and at relatively low cost.4
While a wide variety of organic hole-transport materials
(p-type semiconductors) for applications such as OTFTs
have been successfully developed, electron-transport materi-
als (n-type semiconductors) still have to overcome many
challenges. When highly charged, organic n-type materials
are reactive toward oxygen and moisture, thus making it
Our approach to developing metal-containing perylene
diimide analogues (Scheme 1) involves placing a salpen
ligand (salicyaldehydes connected through a 1,3-propylene-
diamine backbone) betweentwonaphthalimide moieties with
(5) Bao, Z.; Lovinger, A. J.; Dodabalapur, A. Appl. Phys. Lett. 1996, 69,
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(6) Babel, A.; Jenekhe, S. A. Adv. Mater. 2002, 14, 371.
(7) Sirringhaus, H.; Tessler, N.; Friend, R. H. Science 1998, 280, 1741.
(8) Zhu, Y.; Yen, C.-T.; Jenekhe, S. A.; Chen, W.-C. Macromol. Rapid
Commun. 2004, 25, 1829.
(9) Hosoi, Y.; Tsunami, D.; Ishii, H.; Furukawa, Y. Chem. Phys. Lett.
2007, 436, 139.
*To whom correspondence should be addressed. E-mail: bholliday@
cm.utexas.edu.
(10) Kim, K.; Kwak, T. H.; Cho, M. Y.; Lee, J. W.; Joo, J. Synth. Met.
2008, 158, 553.
(11) Chesterfield, R. J.; McKeen, J. C.; Newman, C. R.; Ewbank, P. C.; da
Silva Filho, D. A.; Bredas, J.-L.; Miller, L. L.; Mann, K. R.; Frisbie, D. C. J.
Phys. Chem. 2004, 108, 19281.
(12) Liang, B.; Zhang, Y.; Wang, Y.; Xu, W.; Li, X. J. Mol. Struct. 2008,
917, 133.
(1) Horowitz, G. J. Mater. Res. 2004, 19, 1946.
(2) Organic Electronics: Materials, Manufacturing and Applications;
Klauk, H., Ed.; Wiley-VCH: New York, 2006.
(3) Newman, R. C.; Frisbie, C. D.; da Silva Filho, D. A.; Bredas, J.-L.;
Ewbank, P. C.; Mann, K. R. Chem. Mater. 2004, 16, 4436.
(4) Organic Field-Effect Transistors; Bao, Z., Locklin, J., Eds.; CRC Press:
Boca Raton, FL, 2007.
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2010 American Chemical Society
Published on Web 06/29/2010
pubs.acs.org/IC