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7/31/2019 3,4-Ethylenedioxythiophene (EDOT) as a Versatile Building Block For
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3,4-Ethylenedioxythiophene (EDOT) as a versatile building block foradvanced functional p-conjugated systems
Jean Roncali,* Philippe Blanchard and Pierre Frere
Received 5th October 2004, Accepted 24th December 2004
First published as an Advance Article on the web 31st January 2005DOI: 10.1039/b415481a
The potentialities offered by EDOT as a building block for the synthesis of functional
p-conjugated systems are reviewed. The first part underlines the specific advantages of the
EDOT unit for the design of precursors of electrogenerated functional conducting polymers
combining high reactivity and low polymerization potential. This topic is illustrated by some
recent examples of polymers with specific electrochemical properties and/or a reduced band gap.
The second part is focused on the interest of EDOT as a building block for the synthesis of
various classes of molecular functional p-conjugated systems. Examples of fluorophores, push
pull chromophores for nonlinear optics and extended p-donors are presented. Emphasis is placed
on the optical and crystallographic structure of these compounds, which shows that a major
advantage of the EDOT building block lies in an unique combination of strong electron donor
properties and self-structuring effects related to intramolecular non-covalent interactions between
oxygen and sulfur. Such intramolecular interactions also exert a determining influence on the
structure and electronic properties ofp-conjugated oligomers incorporating EDOT units which
represent some of the more recent uses of the EDOT building block. The structureproperty
relationships of various classes of EDOT-containing conjugated oligomers are discussed in
relation to their potential use as organic semi-conductors. In a brief last section, various synthetic
approaches devoted to the chemistry of EDOT itself, or to the modification of its chemical
structure, are discussed in relation with possible future research directions.
Introduction
During the past two decades, research on functional
p-conjugated systems has rapidly grown as a broad
Jean Roncali was born in Paris in 1949. He received hiseducation in chemistry at the Conservatoire National des Arts etMetiers. He received his PhD from the University of Paris 13
under the supervision of Francis Garnier. After successivepositions as an engineer and Charge de Recherche at CNRS,he is currently Directeur de Recherche at CNRS and head of theLinear Conjugated Systems group at the University of Angers.
His research interests encompass the development of organicmolecules and materials with tailored electronic properties in
view of applications in energy conversion, electronic and photonicapplications and nanodevices.
Philippe Blanchard was born in Vendee, France in 1967.He received his PhD in 1994 from the Universities ofNantes and Angers under the supervision of Professors
G . D ug u ay a n d A . G o rg u es ; h i s s u bj ec t c on ce r ne d tetrathiafulvalene-based molecular materials. He spent one
year as a postdoctoral fellow in the group of Jan Becher atthe University of Odense (Denmark) where he developed
macropolycyclic electroactive compounds. In 1995, hejoined the group of Jean Roncali in Angers as Charge de
Recherche at CNRS to develop thiophene-based pi-conjugatedoligomers and polymers. He obtained his Habilitation in
2001 . His current research int erests concern
the design of pi-conjugated systems for organicelectronic devices.
Pierre Frere was born in Laval, France in 1961.
He received his PhD in organic chem istryfrom the University of Angers in 1993, under thesupervision of Professor A. Gorgues. He then
became Matre de Conferences at the Universityof Angers, where he was promoted to Professorin 1999. His research interests cover various
classes of organic materials derived from tetrathiafulvalene analogues, oligothiophenes and
poly(thiophene)s for electronic applications andmolecular conductors.(Left to right) Philippe Blanchard, Jean Roncali and Pierre Frere
FEATURE ARTICLE www.rsc.org/materials | Journal of Materials Chemistry
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multidisciplinary field extending from theoretical chemistry to
organic chemistry, electrochemistry, photophysics, solid-state
physics and device implementation.1
The discovery of the metal-like conductivity in oxidized
poly(acetylene) or shortly after in polyaromatic systems
such as poly(pyrrole), poly(thiophene) or poly(aniline) in the
late seventies and early eighties,15 has progressively generated
a rich synthetic chemistry in the more general context offunctional p-conjugated systems.
As for conducting polymers in general, the synthetic
chemistry of linearly p-conjugated systems has developed
considerably in the past twenty years and been subject to great
diversification in terms of objectives and methods. During the
period 198090, corresponding to the early developments in
the field, conducting polymers were essentially considered for
bulk applications such as conducting materials for anti-static
coatings, EMI shielding or as electrode materials for energy
conversion and storage. However, after several years of
intensive research effort, it became clear that the insufficient
stability of the charged conducting state of conjugated
polymers represented a major obstacle for further industrialdevelopment.
In 1990, the realization of the first electroluminescent
devices, in which a p-conjugated polymer was used as lumino-
phore by Friend and coworkers, represents a turning point in
the field of p-conjugated systems.6,7 This discovery, together
with a parallel intensification of research on field-effect
transistors8,9 and photovoltaic cells based on p-conjugated
polymers and oligomers,1012 strongly contributed to build up
a quite different vision of linear p-conjugated systems.
With the emergence of the concept of plastic, soft or
flexible electronics p-conjugated systems are no longer viewed
as bulk materials associated with mass industrial production
but as organic semi-conductors synthesized and employed at amuch smaller scale. In this regard, the considerable develop-
ment of nanosciences and molecular electronics in the past few
years, and the emergence of problems related to the design and
synthesis of nano-objects such as molecular wires, switches or
dynamic devices, has further emphasized this molecular vision
of functional p-conjugated systems
In the historical context of the 198090 period, the chemistry
of conducting polymers can be roughly qualified as an
additive side chain approach, with as main goal the addition
of new properties such as solubility, hydrophilicity, or
molecular recognition to the inherent electronic, optical or
electrochemical properties of the conjugated backbone of
polymers such as poly(pyrrole) or poly(thiophene) by covalentfixation of functional side groups.15,13
The emergence of plastic electronics has generated a quite
different view of the chemistry of functional p-conjugated
systems and the control and manipulation of quantities such
as absorption and emission spectra, oxidation and reduction
potentials or luminescence efficiency became the new priority
targets.
At the begining of the 90s, chemists at the Bayer company
described a novel conducting polymer poly(3,4-ethylenedioxy-
thiophene) (PEDOT). Owing to several distinct advantages,
PEDOT rapidly acquired a prominent position among con-
ducting polymers. A unique combination of moderate band
gap and low oxidation potential confers on PEDOT an
exceptional stability to the oxidized charged state which
furthermore exhibits high conductivity and good optical
transparency in the visible spectral region.1416 Based on these
properties many applications of PEDOT have been rapidly
developed including anti-static coatings, electrode material
in supercapacitors or hole injection layer in OLEDs and
solar cells.
12,1720
Although PEDOT was initially viewed as a novel conduct-
ing polymer, it became rapidly clear that the EDOT molecule
itself presented some specific chemical properties which made
it an interesting building block for the synthesis of functional
p-conjugated systems. In fact, in addition to their strong
electron donor effect, the ether groups at the b,b9 positions of
thiophene ring prevent the formation of parasitic ab9 linkages
during polymerization while conferring a high reactivity to
the free a,a9 positions. During the past decade, these properties
have been widely used to synthesize various classes of
electrogenerated polymers combining some of the specific
properties of PEDOT to original electrochemical or optical
properties. These various aspects of the electro-optical andelectrochemical properties of EDOT-based polymers have
already been subject to two review articles.19,20 However,
beyond the synthesis of functional conducting polymers,
EDOT also represents a unique building block for the design
of various classes of molecular p-conjugated systems with
electronic and optical properties specifically tailored for
applications in light-emitting devices, chromophores for non-
linear optics, low energy gap systems or more recently organic
semi-conductors.
This increasing attention for EDOT-based systems has in
turn generated a strong interest in the chemistry of the EDOT
molecule itself and/or in the modification of its structure.
In this general context, the aim of this short review is not topresent a comprehensive survey of the synthesis and applica-
tions of PEDOT and its derivatives, but rather to emphasize
the opportunities offered by the EDOT building block for the
design and synthesis of new classes of functional p-conjugated
systems.
1. EDOT as a building block for the design of
precursors of functional p-conjugated polymers
The electropolymerization of substituted precursors represents
a simple and straightforward method for the elaboration of
modified electrodes in which the inherent electrochemical
and electronic properties of the p-conjugated backbone areassociated with specific properties brought by the covalent
fixation of a functional group on the monomer.21,22 During the
past two decades modified electrodes based on this concept
have represented a major topic in the chemistry of conducting
polymers. Initially focused on the conversion and storage
of electrical energy23,24 or electrochromic devices,25,26 the
field has progressively evolved towards more sophisticated
systems such as electrode materials for electrocatalysis and
(bio)electrochemical sensors.21,22,27
Despite its conceptual simplicity, the synthesis of functional
electrogenerated conducting polymers poses several complex
problems related to the direct and indirect effects of the
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attached functional group on the polymerization reaction
and on the structure and properties of the resulting polymer.
Thanks to the intensive research effort invested in this
area during the 80s, rules for the molecular engineering of
functional conjugated polymers have progressively emerged
with, in particular, the need to introduce a spacer between
the functional group and the p-conjugated chain in order to
minimize electronic and steric effects of the substituents onthe polymerization process, and on the effective conjugation
length of the resulting polymer.13,21
Besides pyrrole-based systems, which will not be discussed
here,27 most of the functional conducting polymers of the first
generation have been obtained by electropolymerization of
precursors in which a functional group is attached at the
3-position of a thiophene ring through an appropriate spacer
group. In general, a spacer involving at least two carbons
allows the neutralization of the electronic effects of most
electron-releasing or -withdrawing groups on the reactivity
of the thiophene ring.13 However, in the case of bulky sub-
stituents longer spacers may be needed to reduce steric
interactions between substituents and to preserve the planarityof the p-conjugated backbone.21
Although widely applied, the scope of this approach is
limited by the highly positive potential required to electro-
oxidize 3-alkythiophenes or functionalized monomers of
related structure. In fact, when the oxidation potential of
the functional group is significantly lower than that of the
thiophene, various kinds of deleterious effects can be expected,
namely, (i) a large part of the anodic current will be consumed
in the oxidation of the side substituent leading to its eventual
irreversible degradation, and (ii) the attached functional group
can act as a scavenger for thiophene cation radicals and thus
inhibit the electropolymerization process.28,29
A first possible way to decrease the oxidation potential of
the precursor consists of replacing thiophene by a longer
oligomer with lower oxidation potential. However, the pro-
gressive decrease in the reactivity of the cation radical as chain
length increases13,30 severely limits the scope of this approach.
In fact, as exemplified in the case of the poly(thiophenes)
functionalized by crown ethers, synthesized by Bauerle and
coworkers,
31
bithiophenic systems seem to represent the besttrade-off between the decrease of the polymerization potential
and the preservation of a sufficient reactivity of the cation
radical.
In this context, the specific electronic properties of EDOT,
in terms of reactivity and donor effect, represent interesting
tools for the design of precursors combining the low electro-
polymerization potential and high reactivity of the cation
radical.
A widely-used approach, initially developed by Reynolds
and coworkers, involves the synthesis of hybrid tricyclic
precursors in which a functional block, eventually possessing
specific electronic, chemical or electrochemical properties, is
inserted between two EDOT groups (Scheme 1).32
In thepast decade this in chain approach has been widely applied
to the synthesis of many precursors with a median block
extending from simple moieties, i.e. double bonds (1),33
thiophenes (2), furans (3), benzenes (4),32 substituted thio-
phenes,34 or pyridines (5),35 to larger systems such as biphenyls
(6),32 bipyridines (7),36 fluorenes (8),37 carbazoles (9),38 N,N9-
ethylene-bis-(salicylideimine) metal complexes (10),39,40 or
tetrathiafulvalenes (11).41
A major advantage of this approach is that the high
reactivity of the lateral EDOT groups makes it possible to
electropolymerize precursors in which the central block limits
or even interrupts electron delocalization along the polymer
Scheme 1 Examples of in chain functionalized EDOT-based conjugated polymers.
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hydrophilic polymers possess the unique ability to undergo
fast solid-state ionochromism when immersed in solutions of
various metal ions, or immediate contraction of band gap
when immersed in water. Finally, a comparative analysis of
the cyclability of the polymers showed that the polymers
synthesized from the two-site precursors 18 are considerably
more stable under long-term repetitive redox cycling than
their analogs derived from the singly substituted-EDOTmonomer 17.47
In addition to their rather complex synthesis, functionalized
monomeric EDOT precursors exhibit an oxidation potential
similar to that of EDOT (ca. 1.70 V vs. SCE), which still
represents a major obstacle for the electropolymerization
of precursors containing sensitive functional groups. For
example, in the specific case of compound 14, the considerably
lower oxidation potential of ferrocene relative to that of
EDOT renders the electropolymerization very difficult. Con-
sequently, stable ferrocene-derivatized polymers were only
obtained by co-polymerization with other EDOT derivatives.45
In order to define an optimal trade-off between reactivity
and the lowered polymerization potential we have recentlydeveloped a new class of precursors based on the EDOT
thiophene structure in which the functional group is attached
by formation of an electron releasing sulfide or ether group.
Substituted thiophene monomers based on a 3-alkylthio-
phene structure present an oxidation potential of ca. 1.80 V vs.
SCE and require a minimal concentration of 0.10 M in order
to produce electrodeposited polymer films of good quality.13,21
As already indicated, replacing thiophene with bithiophene
allows the reduction of the polymerization potential to 1.30 V
vs. SCE and the minimal concentration to about 1022 M.31,48
A further improvement was achieved in 1997, when we showed
that replacement of thiophene by EDOT in bithiophenic
precursors permitted a further decrease of the electropoly-merization potential to 1.15 V. This kind of precursor proved
to be particularly effective for the electrosynthesis of tetra-
thiafulvalene-derivatized poly(thiophenes).48,49 However, like
many of the 3-substituted functionalized thiophenic pre-
cursors, these improved bithiophenic systems were still based
on the 3-(v-halogenoalkyl)-thiophenes prepared according
to the method described by Bauerle.50 Despite its interest,
this method presents several important limitations, namely
(i) it requires multiple synthetic steps, (ii) final deprotection of
the halide group requires drastic conditions which are not
applicable to longer oligomers or to polymers and (iii) it is not
valid for alkyl chains containing less than four carbons.
In an attempt to solve some of these problems, we havedeveloped alternative methods of functionalization based on
the formation of sulfide or ether groups. In these cases,
functionalization is realized by reacting a functional group
bearing a terminal halogenomethyl moiety onto a 3-thiophene-
thiolate or 3-thiophene-alcoolate. These intermediate
compounds are produced by cleavage of 3-(2-cyanoethyl-
sulfanyl)thiophene or 3-(2-cyanoethyloxy)thiophene under
mild conditions.51,52 These two compounds are easily obtained
from 3-bromothiophene or 3-methoxythiophene respectively
(Scheme 2). An advantage of the cyanoethyl protected group is
that it can be engaged in further chemistry to synthesize hybrid
EDOT-based precursors. Furthermore, in addition to an easy
and rapid method of functionalization, the strong electron-
donor effect of the thus formed sulfide or ether group produces
a further decrease in the oxidation potential of the bithiophe-
nic precursor.With these new hybrid EDOT-based bithiophenic systems it
is now possible to efficiently electropolymerize functionalized
precursors at potentials lower than 0.90 V vs. SCE and sub-
millimolar concentrations.52 This recent progress in the design
of precursors enables researchers to envision the synthesis
of more elaborated functional polymers or to reconsider the
design of polymers which proved to pose specific problems in
the past.
Thus, although several groups have reported attempts to
synthesize poly(thiophenes) containing bipyridyl ligands and
some of their metal complexes, conclusive evidence for the
efficient electrosynthesis of well-defined stable and extensively
conjugated polymers has not been reported until now.21
Therefore, one of the first applications of the newly designed
low oxidation potential bithiophenic precursors has involved
the synthesis of bipyridine-derivatized conjugated polymers.
To this end, precursors 19 and 20 in which two EDOT-based
hybrid bithiophene groups are attached on a bipyridine have
been synthesized. As shown in Fig. 1, the combination of these
low oxidation potential precursors with the already discussed
advantages of the multi-site approach allows a straight-
forward electropolymerization to form stable and extensively
p-conjugated polymers containing bipyridine ligands.52
In the next step, various transition-metal complexes contain-
ing two to six hybrid EDOTthiophene groups (2123) were
Scheme 2 Synthesis of low polymerization potential precursors.
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synthesized and electropolymerized. Thus, the cyclic voltam-
mogram of poly(23) shows a first reversible redox system
around 0.60 V characteristic of an extensively conjugated
poly(thiophene) backbone followed by a reversible anodic
wave at 1.00 V typical of the [Fe(Bipy)3]2+/3+ redox couple.
In the negative potential region, the CV shows the two
successive redox systems associated with the [Fe(Bipy)3]2+/+
and [Fe(Bipy)3]
+/0
redox couples (Fig. 2).
52
Another recent application of the same strategy has
involved the synthesis of poly(thiophenes) containing pendant
C60-fullerene groups. Such materials have been essentially
developed in view of their potential use as active materials
in organic solar cells.53 Precursors 24 and 25, containing one
and two polymerizable groups respectively, have been synthe-
sized using successively thiophenethiolate chemistry and the
Bingel reaction.54,55
Comparison of the cyclic voltammograms corresponding to
the potentiodynamic electropolymerization of compounds 24
and 25, shows that the two site-precursor 25 leads to a faster
increase of the less positive anodic wave around +0.30 V,
which is indicative of the growth of a more conjugated polymer(Fig. 3). This conclusion has been confirmed by the analysis of
the electrochemical and optical properties of the two polymers.
Furthermore, chronoamperometric experiments carried out on
the two polymers have shown that for the same film thickness,
poly(25) exhibits a much faster response to a potential step, in
agreement with the expected more porous structure.55
Fig. 1 Potentiodynamic electropolymerization of compound 19 (top)
and 20 (bottom), 1 mM in 0.10 M Bu4NPF6CH2Cl2, 100 mV s21, Pt
electrodes. (From ref. 52, reproduced by permission of The Royal
Society of Chemistry.)
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Preliminary tests of the photoelectrochemical response of afilm of poly(25) on a platinum electrode (Fig. 4) showed that
the photogenerated current is ca. three times larger than that
obtained under the same conditions with a reference parent
polymer in which the C60 group of poly(25) is replaced by an
hexyl chain linking the two sulfide groups. This result thus
underlines the potentiality of this new class of functional
conjugated polymers for photovoltaic conversion.55,56
Compounds 26 and 27 represent the first members of
another interesting class of compounds combining EDOT and
fullerene C60. These compounds present the particularity to
form self-assembled monolayers (SAMs) on gold surfaces.57
The resulting SAMs are quite stable and exhibit unchanged
CV after several weeks storage under ambient atmosphere. The
cyclic voltammogram of a SAM of compound 27 at various
scan rates shows two successive waves corresponding to the
reduction of C60 into its anion radical and dianion (Fig. 5).
The linearity of the plot of the current peak with scan rate
confirmed that the reduction corresponds to a surface-
confined electrochemical reaction.
No change in the CV is observed under repetitive cycling in
the negative potential region (down to 21.80 V vs. Ag/AgCl).However, a particularly interesting property of these SAMs
is that they can be electrochemically desorbed from the
electrode surface by anodic oxidation of the attached EDOT
or bi-EDOT group.57
2. EDOT as a tool for molecular engineering of the
energy gap ofp-conjugated systems
Most of the relevant electronic properties of p-conjugated
systems depend on the energy level of the frontier orbitals and
the difference between them. Consequently, the control of the
HOMOLUMO gap (DE) of conjugated systems and of the
Fig. 2 Cyclic voltammogram of poly(23) in 0.10 M Bu4NPF6
CH3CN, scan rate 100 mV s21. (Reprinted from ref. 52, reproduced
by permission of The Royal Society of Chemistry.)
Fig. 3 Potentiodynamic electropolymerization of compound 24 (top),
and 25 (bottom) 1 mM in 0.10 M Bu4NPF61 : 4 CH3CNCH2Cl2,
100 mV s21. (Reprinted from ref. 55, Copyright 2003, American
Chemical Society.)
Fig. 4 Variation of the photocurrent under polychromatic irradia-
tion of polymer films electrodeposited on platinum electrodes, (black)
reference polymer (see text) (red) poly(25). Polarization 20.10 V vs.
Ag/AgCl) in 0.10 M Bu4NPF6CH3CN. (Reprinted from ref. 55,
Copyright 2003, American Chemical Society.)
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band gap (Eg) of the resulting molecular or polymeric
materials has progressively become a major topic for the
chemistry of functional p-conjugated systems.58 The HOMO
LUMO gap of a linear p-conjugated system depends on
various structural factors such as chain length, bond length
alternation, planarity, the presence of electron-acceptor or
electron donor substituents and the resonance stabilization
energy of the aromatic cycles. Although not fully independent,
these various factors represent possible synthetic approaches
for gap engineering such as the grafting of donor and/or
acceptors groups on the conjugated backbone, the searchfor systems with a quinoid ground state, or the rigidification
of the conjugated structure in order to improve planarity and
to reduce bond length alternation.58
In this context, the strong electron donor properties
of EDOT represent an interesting tool for the molecular
engineering of the band gap of p-conjugated systems. One
of the simplest ways to take advantage of these properties
is to associate EDOT with electron withdrawing groups by
synthesizing copolymers. Thus Huang and Pickup have
reported that electrochemical copolymerization of EDOT and
4-dicyanomethylene-4H-cyclopenta[2,1-b;3,4-b9]dithiophene
(28) led to a copolymer for which a very low band gap
was claimed.59
More recently, Wudl and coworkers havesynthesized another low band gap copolymer using a Stille
reaction between di-stannyl-EDOT and the dibromo
derivative of thienyl-benzo[c]thiophene-N-20-ethylhexyl-4,5-
dicarboximide (29) (Scheme 3). The copolymer showed
electrochromic properties in the IR region.60
The possibility to tune the gap, and hence the optical pro-
perties, of EDOT-containing block co-polymers was initially
investigated by Reynolds and coworkers, who reported many
examples of in chain functionalized co-polymers obtained
by electropolymerization of tricyclic precursors. In this case,
gap modulation was achieved by changing the chemical nature
of the median group (Scheme 1).19,20
More drastic reduction of the band gap of poly(thiophene)
can be achieved by introduction of electron acceptor groups
on the conjugated backbone.
21,58
As shown already forpoly(p-phenylene),61,62 and thiophene-based systems,63,64 the
grafting of cyano groups at the ethylene linkage connecting
two phenyl or thiophene rings represents a simple and efficient
method for gap reduction. Furthermore cyano groups can
be easily introduced at a vinylene linkage by Knoevenagel
condensation.6165 Thus, precursors 30 and 31 have been
prepared by condensation of 2-formyl-EDOT with the appro-
priate thiophene-acetonitrile. Electropolymerization of these
compounds led to polymers with band gaps smaller than
1.50 eV.65,66
Until now, p-conjugated polymers with the smallest band
gaps have been obtained by electropolymerization of tricyclic
systems in which two donor side groups such as pyrrole orthiophene are attached to a median fused ring system which is
as the same time a strong electron acceptor and a proquinoid
system. This strategy has been extensively developed by
Yamashita and coworkers who used many examples of pro-
quinoid acceptor groups.58,67,68
More recently, our group has extended this approach to
several tri-block systems in which EDOT serves as side donor
group. Thus tricyclic systems based on thieno[3,4-c]-pyrazine
(32),6971 benzo[3,4-c]thiophene (33),69,72 benzothiadiazole
(34)72 or thienothiadiazole (35)69 have been synthesized as
precursors of low band gap polymers. As shown by the X-ray
structure of compound 32, the molecule adopts a fully planar
geometry (Fig. 6). Furthermore, examination of the non-bonded distances between sulfur and oxygen or nitrogen and
oxygen atoms of the adjacent cycles shows that the sulfur
nitrogen and sulfuroxygen distances are markedly smaller
than the sum of the van der Waals radii of the individual
atoms, thus demonstrating the existence of non-covalent
intramolecular interactions which contribute to planarize the
system. Thus, in addition to the electronic effects already
observed in the tricyclic systems synthesized by Yamashita and
coworkers, EDOT introduces a self-structuration effect which
contributes to a further reduction of the gap. Comparison of
the electronic absorption spectra of compounds 3235 to those
of terthienyl reveal considerable red shifts of the absorption
Fig. 5 Cyclic voltammograms of a SAM of 27 in 0.05 M Bu4NPF6 in
o-dichlorobenzene, scan rate 100 to 1000 mV s21. (From ref. 57,
reproduced by permission of The Royal Society of Chemistry.)
Scheme 3 Synthesis of low band gap copolymers.
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maximum indicative of the reduction of the HOMOLUMO
gap. Electropolymerization of tricyclic compounds 3235 leads
to polymers with band gaps in the range of 1.101.30 eV. 6973
Lee et al. recently reported the synthesis and electropoly-
merization of a related system involving a median 3,4-
diphenylsilole (36). The optical spectrum of the obtained
polymer indicated an estimated band gap of 1.301.40 eV.74
Wudl and coworkers have described the synthesis of 1,3-bis(29-[39,49ethylenedioxy]thienyl-benzo[c]thiophene-N-20-ethylhexyl-
4,5-dicarboximide (37). The resulting electrogenerated polymer
presented an optical band gap of 1.10 eV and was reported
to be very stable in both the oxidized and reduced forms. 75
Cyclopenta[2,1-b;3,4-b9]dithiophene-4-one and 4-dicyano-
methylene-4H-cyclopenta[2,1-b;3,4-b9]dithiophene are well-
known precursors of low band gap polymers.7578 Berlin et al.
have recently synthesized compounds 38 and 39 in which
EDOT groups are connected at both ends of these electron
acceptor bithiophenic systems. Electrochemical and optical
data provided consistent results showing that these polymers
present band gaps of 0.801.30 eV.79
Although these various results confirm the interest of the
association of EDOT with proquinoid acceptors, the reported
values of the band gap remain in the whole rather large. For
Fig. 6 Crystallographic structure of compound 32 (from ref. 69).
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example the band gap of poly(33) is still comparable to that of
the homopolymer of benzo[c]thiophene initially described by
Wudl et al.80 This result can be attributed to two causes. On
the one hand, polymerization of tricyclic precursors leads to
bis-EDOT sequence alternating with acceptor group and it is
likely that optimal gap reduction requires a regular alternation
of donor and acceptor groups.58,81 On the other hand, and as
already discussed, oligomeric precursors are in general moredifficult to polymerize efficiently due to the limited reactivity
of their cation radicals.13,30 Indeed, conclusive evidences for
incomplete electropolymerization have been obtained in the
case of poly(33), for which the CV recorded in a monomer-free
electrolytic medium reveals a negative shift of the anodic peak
upon repetitive cycling, a phenomenon characteristic for the
coupling of unreacted precursor molecules trapped in the
polymer during electrodeposition.82
In this regard, the use of di-block systems in which EDOT is
associated with a proquinoid thiophenic acceptor present
distinct advantages related to (i) the higher reactivity of
bithiophenic precursors and (ii) the difference in reactivity of
the terminal a-positions of EDOT and thiophene which allowsthe formation of a regular alternation of donor and acceptor
blocks after an initial EDOTEDOT coupling. These effects,
associated with the non-covalent self-rigidification observed in
the model compound 32, could explain the very small band
gap of the polymer obtained by electropolymerization of the
EDOT-thieno[3,4-b]pyrazine precursor (40) which reaches one
of the smallest values know to date (Eg, 0.40 eV) and exhibits
an exceptional stability under repetitive n-doping cycling.83
This considerable decrease of Eg compared to poly(32)
(1.10 eV) can be attributed to the combined effects of regular
alternation of donor and acceptor groups, to the already
mentioned incomplete polymerization of tricyclic systems such
as 32 or 33 and to the self-rigidification of the structure by non
covalent intramolecular interactions. On the other hand, the
unusual stability under long-term n-doping cycling suggeststhat a dense packing of the polymer chains may limit oxygen
permeation in the polymer bulk. Such a tight packing, which
also contributes to reduce the band gap, can also explain the
complete insolubility of the polymer despite the presence of
two hexyl chains on the pyrazine ring.
In order to improve the solubility of this type of structure we
have recently synthesized a parent precursor in which EDOT is
substituted by an n-decyloxy chain grafted at the ethylenedioxy
bridge (41). Comparison of the electrochemical and optical
properties of the resulting polymer to those of poly(40) reveals
a 0.35 V negative shift of the peak potential corresponding to
the n-doping and a considerable decrease of stability under
reductive cycling. Furthermore, comparison of the optical
spectra of the neutral polymers shows that lmax shifts
hypsochromically from 1460 nm for poly(40) to 1070 nm for
poly(41), which corresponds to an increase of the band gap
from 0.40 to ca. 0.80 eV (Fig. 7).84 These unexpected results
are in fact the consequences of the introduction of the decyl
substituent at an sp3 carbon of the ethylenedioxy bridge. This
implies that the location of the solubilizing alkyl chain above
or below the plane of the p-conjugated polymer backbone
significantly increases interchain distance and hence decreases
p-stacking interactions. This situation is in total contrast with
the case of poly(3-alkylthiophenes) for which p-stackinginteractions between conjugated chains are possible since the
alkyl chains are attached at a sp2 carbon of the thiophene ring.
Thus, in poly(41) the grafting of the decyl chain contributes
at the same time to increase the band gap by hindering
intermolecular p-stacking interactions and to decrease the
stability of the reduced form of the polymer due to an easier
oxygen permeation in the bulk material.
These results show that despite the high interest of EDOT
for band gap engineering, its solubilization poses specific
problems which require the definition of appropriate synthetic
strategies.
3. EDOT-based functional p-conjugated systems forelectro-optical applications
The combination of the strong electron-donor and self-
structuring effects of EDOT also represent powerful tools for
the design and synthesis of molecular functional p-conjugated
systems for various optical and electro-optical applications.
Thus, in addition to their use as precursors of low band gap
polymers, tricyclic compounds such as 33 and 34 present a
unique combination of electronic properties which make
them potentially interesting as fluorophores for light-emitting
devices. As shown in Table 1, compared to a terthienyl
reference (3T) these compounds exhibit lower oxidation
Fig. 7 Spectroelectrochemistry of a poly(41) in 0.10 M Bu4NPF6
CH3CN. Electrodeposited on a 5 mm diameter Pt disk. (From ref. 84,
reproduced by permission of The Royal Society of Chemistry.)
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potentials, positively shifted reduction potentials and very high
fluorescence quantum yields.72
More recently, other EDOT-based tricyclic compounds
based on median groups such as substituted thiophenes (42),substituted phenyls (43), thiazoles (44) or oxadiazoles (45)
have been proposed as photoluminescent materials.34,8587
However, as shown in Table 1, the reported luminescence
quantum yields remain in general low and comparable to that
of terthiophene.
From a different viewpoint, compound 47 has been recently
shown to exhibit a dramatic enhancement of fluorescence in
the presence of pyrophosphate anions.88
Thiophene-based systems have been widely used as
p-conjugating spacers in pushpull chromophores designed
for 2nd order nonlinear optics.89 In this context, we have
synthesized various series of pushpull NLO-phores in which
thiophene (48) or bithiophene (50) have been replaced by
EDOT (49) or bis-EDOT (5153) as conjugating spacers.90,91
The optical data in Table 2 show that, as expected, the increase
of the acceptor strength in the 5153 series leads to a
bathochromic shift of lmax accompanied by an increase of
the quadratic hyperpolarisability (mb). Comparison of the datafor compound 48 and 49 shows that despite a 78 nm red shift
oflmax, replacement of thiophene by EDOT produces in fact a
decrease ofmbwhich is partly due to a decrease of the dipole
moment of the pushpull system.90
On the other hand, comparison of the efficiency of
compounds 5153 to that of other systems based on the same
donoracceptor couple but containing different conjugating
spacers shows that the bis-EDOT spacer leads to an efficiency
comparable to that of dithienylethylene (DTE) but inferior to
that of bridged DTE.91,92
However, comparison of the data for compounds 50 and 53
which contain the same donoracceptor couple clearly shows
that replacement of the bithiophene by the bis-EDOT con-jugating spacer produces a 118 nm red shift of lmax and
more than a twofold increase of mb. Contrary to the case of
compounds 48 and 49, replacement of bithiophene by bis-
EDOT does not produce a decrease of the dipole moment, but
on the contrary a slight increase. However since this small
increase of m alone cannot explain the observed strong
enhancement of mb, these results confirm that bis-EDOT is a
more efficient p-conjugating spacer than bithiophene.
The analysis of the crystallographic structure of a single
crystal of the EDOT dimer90,93 provides some interesting
information about the origin of the enhanced p-electron
delocalization observed on pushpull chromophores based
on bis-EDOT. Examination of the non-bonded distancesbetween sulfur and oxygen (Fig. 8) shows that these distances
(2.92 A) are significantly shorter than the sum of the van der
Waals radii of sulfur and oxygen (3.25 A). These short
distances confirm the occurrence of the already discussed
strong intramolecular non covalent interactions which rigidify
the p-conjugated structure in a fully planar anticonformation.
This self-rigidification of the bis-EDOT structure thus signifi-
cantly contributes to improve the electron transmitting
properties of bis-EDOT compared to bithiophene.
In addition to pushpull chromophores, EDOT-based
p-conjugated systems have also been incorporated in various
kinds of donor or acceptor compounds potentially useful for
Table 1 Electrochemicala and optical properties of EDOT basedfluorophores
Compound Epa/V Epr/V lmax abs/nm lmax em/nm wem
3T 1.10 22.00 350 430 0.066b
33 0.56 21.80 450 613 0.920c
34 0.92 21.40 481 630 0.750c
42a 361 441 0.034d
42b 361 441 0.032d
43a 326 413 0.001d
43b 339 397 0.096d
43c 338 440 0.025d
43d 336 410 0.103d
44 377 452 0.054d
45 ,320 413 0.090d
46a 595 629 Nr46b 614 657 Nra In 0.10 M Bu4NPF6MeCN, ref. SCE.
b In dioxane, ref. 128.c Ref. 72. d Quinine sulfate as standard, ref. 86.
Table 2 Absorption maximum,a, quadratic hyperpolarisabilityb, cal-culated dipole moment (m)c, and decomposition temperatured ofchromophores 4853
Compound lmax/nm mb/10248 esu m/D Td/uC
48e 690 6100 9.4 49 768 4600 (1300) 8.0 23050 712 5000 (1900) 15.9 21551 588 2120 (1200) 30852 649 2000 (950) 30053 830 11600 (2400) 17.1 206a In CH2Cl2.
b Measured in CHCl3 at 1.9 mm by the electric field-induced second harmonic generation (EFISH), values in parenthesesrepresent the zero frequency hyperpolarisability product mb0.c Calculated using Gaussian 98 after optimization of the geometries.d Determined in atmospheric conditions by DCS at a rate of10 uC min21. e Ref. 129.
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IR region which were assigned to oligothiophene to Fe(III)charge-transfer transitions.99
4. EDOT-based p-conjugated oligomers
In recent years, monodisperse p-conjugated oligomers have
acquired a growing importance in materials science.100,101
Initially considered as models of the corresponding poly-
disperse polymers, conjugated oligomers have progressively
emerged as a new class of materials with electronic properties
often equalling or even surpassing those of the corresponding
polymers. This point has been illustrated in particular by the
large number of publications in which oligomers are used
as organic semi-conductors for the realization of devicessuch as field-effect transistors or light-emitting diodes.7,9
Consequently, control of the electronic properties of con-
jugated oligomers in view of these advanced technological
applications has become a focus of intensive research effort. In
this context, it is clear that the combined electron donor and
self-structuring properties of EDOT represent an invaluable
tool for the design of new oligomeric structures with tailored
electronic properties.
Because of the high reactivity of the terminal a-positions of
EDOT, the length of pure EDOT oligomers has been until now
limited to rather short-chain systems. The EDOT dimer (61)
was initially synthesized as a low oxidation potential precursor
for electropolymerization.93
Almost simultaneously it wasreported that bis-EDOT end-capped with trimethylsilyl
groups102 could be electropolymerized, as previously estab-
lished for various other thiophenic precursors.103
The EDOT trimer (62) was first synthesized by Reynolds
and coworkers as a precursor for electropolymerization.32
However this compound was described as very unstable. This
instability, attributed to the high reactivity of the terminal
a-positions of ter-EDOT has led several groups to synthesize
end-capped EDOT oligomers.104106
Hicks and Nodwell first reported the synthesis of di-and ter-
EDOT end-capped with mesitylthio groups (63, 64) and
analyzed their optical and electrochemical properties. As
expected, the combined donor effects of the EDOT andbis(arylthio) groups produced a significant decrease in the
oxidation potential of the conjugated chain and a red shift of
the absorption maximum compared to oligothiophenes.104
Janssen and coworkers have reported a comparative analysis
of the optical and redox properties of a series of EDOT
oligomers containing one to four EDOT units end-capped with
phenyl groups (65) and of their thiophene based analogs.105
Absorption and fluorescence emission spectra revealed a
markedly higher degree of intra-chain order in EDOT
oligomers. Electrochemical data confirmed the lower oxidation
potential of EDOT oligomers compared to oligothiophenes.
Linear plots of the oxidation potential vs. the reciprocal chain
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length revealed significantly steeper slopes for oligo-EDOTs,
suggesting a more effective conjugation for a given chain
length. Extrapolation of the first and second oxidation
potentials suggests that coalescence of the two oxidation steps
should occur at a shorter chain length for EDOT oligomers
than for oligothiophenes.105
More recently, our group has described a series of EDOT
oligomers end-capped with n-hexyl chains and containing one
to four EDOT units (66).106 As shown in Fig. 9, the electronic
absorption spectra of these oligomers in dichloromethanesolutions present a well-resolved vibronic fine structure
consistent with a planar and rigid conjugated system.
As already discussed at several instances, this self-structur-
ing effect results from intramolecular interactions between
sulfur and oxygen atoms of adjacent EDOT units. Again these
interactions are clearly apparent in the crystallographic struc-
ture of the 66 series trimers.106
The cyclic voltammograms of the 66 series oligomers show
that the trimer and tetramer can be reversibly oxidized into
their cation radical and dication state. Linear plots of the two
oxidation potentials vs. the reciprocal chain length indicate
that coalescence of the two oxidation steps should occur for an
infinite chain length. This conclusion, which contradicts that
drawn by Janssen and co-workers for their phenyl-cappedEDOT oligomers,105 suggests that in this latter case, the
terminal phenyl groups contribute to the charge delocalization
which is, of course, not the case for our n-hexyl end-capped
oligomers.
Hybrid oligomers
Because of the strong electron donor properties of EDOT, the
maximum chain length of oligo-EDOTs has remained so far
limited to the tetramer, whatever the nature of the terminal
blocking group.104106 A possible way to circumvent this
obstacle can consist of the combination of EDOT with other
building blocks in order to reach more extended conjugatedchain lengths.
The first EDOT-containing conjugated oligomers were
reported in 1999 by Cava and coworkers who described the
synthesis of hybrid systems based on various combinations of
EDOT and vinylene linkages (6769) and the hybrid EDOT
thiophene tetramers 72 and 73.107 Shortly after we described
the synthesis and electrochemical and optical properties of
the thienylenevinylene hybrid systems 70 and 71, and a new
synthesis of tetramers 72 and 73.108
The analysis of the electrochemical properties of compounds
7073 shows that when the two EDOT groups occupy the
inner positions of the molecule, the cyclic voltammogram
Fig. 9 Electronic absorption spectra of EDOT oligomers 66 (n = 2, 3,
4) in CH2Cl2. Short dashed line, n 5 1; long dashed line, n 5 2; solid
line, n 5 3. (Reprinted from ref. 106, Copyright 2003, American
Chemical Society.)
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MesS groups which cause charge density in the cation radical
to concentrate at the chain ends thus lowering the Coulombic
barrier to the introduction of a second charge.104
Recently, we have carried out a systematic analysis of
the structureelectronic property relationships in three series
of hybrid oligomers end-capped with n-hexyl chains and
based on various combinations of thiophene and EDOT
groups (7785).
109
The analysis of the crystallographic structure of two hybrid
quaterthiophenes 77 and 78 by X-ray diffraction shows that
when the EDOT group occupy the outer positions, the two
inner thiophenes adopt a syn conformation with a 13u dihedral
angle. In contrast insertion of a bis-EDOT block in the middle
of the molecule leads to an all-anti fully planar conformation
stabilized by strong intramolecular SO interactions (Fig. 11).
UV-Vis absorption spectra show that increasing the number
of EDOT groups in the structure leads to a red shift of the
absorption maximum with an exaltation of the vibronic fine
structure. This latter effect, indicative of a rigid p-conjugated
structure, strongly depends on the position of the EDOT
groups and becomes particularly intense when adjacent EDOTgroups are inserted in the middle of the molecule. Nevertheless
the vibronic fine structure persists in alternated oligomers and
the fact that it is still discernible in the heptamer indicates that
the coherence length of the intramolecular self-rigidification
associated with the non-covalent SO interactions is at least
equal to seven thiophene units (Fig. 12).
As expected, cyclic voltammetric data show that the first
oxidation potential decreases when increasing the number of
EDOT groups in the structure. However, the position of the
EDOT groups considerably affects the potential difference
(DEp) between the first and second oxidation steps; moving the
EDOT groups from the ends to the middle of the conjugatedsystem produces an increase of DEp. As confirmed by
theoretical calculations, this phenomenon reflects an increase
of the on-site Coulombic repulsion between positive charges in
the dication, since these charges tend to localize in the vicinity
of the electron donor EDOT groups.
In order to obtain a first evaluation of the potentialities of
these hybrid oligomers as organic semi-conductors, a thin
film field-effect transistor has been fabricated by vacuum
sublimation of pentamer 81 with alternated thiopheneEDOT
structure. The OFET was built on an n-doped silicon gate
with thermally grown SiO2 as dielectric. Gold source and
drain electrodes were deposited by sublimation on top of
the organic film through a mask. A hole mobility of 0.6 61023 cm2 V21 s21 has been determined.109 Although modest,
this first result obtained on a single unoptimized device shows
that EDOT-containing conjugated oligomers can be indeed
behave as organic semi-conductors. These preliminary results
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should provide a strong incitement to develop further research
aimed at a better understanding of the structure-electronic
properties of these hybrid oligomers.
Curtis and coworkers have reported the synthesis and
characterization of bis-EDOT-4,49-diakyl-2,29-bithiazole) co-
oligomers (8688) as potential organic semi-conductors.110
The UV-Vis spectrum of the shortest system 87 shows an
absorption maximum at 410 nm, while the spectra of com-
pounds 86 and 88 show the same absorption maximum at
466 nm. The spectra of solution-cast thin films revealed a
bathochromic shift of the absorption band with the appear-
ance of a fine structure which was attributed to the effects of
p-stacking, a point subsequently confirmed by the crystal-
lographic structure.111 Although all oligomers could be
electrochemically oxidized and reduced, the position of the
EDOT groups exerts a marked influence on the cyclic voltam-
mogram. Thus whereas the CV of compound 86 exhibits
a quasi-reversible oxidation wave, the oxidation process of
compounds 87 and 88 is irreversible, presumably because of
the subsequent chemical coupling of the electrogenerated
cation radicals.110 Chemical oxidation of these compounds led
to the sequential formation of the cation radical and dication.
The cation radical was found to form diamagnetic p-dimers.
The allowed pp electronic transition was interpreted in terms
of molecular exciton theory leading to a nearest-neighbor
exciton coupling constant of 0.2 eV.112
5. Modification of the chemical structure of EDOT
As the above-discussed multiple utilizations of the EDOT build-
ing block in functional p-conjugated systems progressively
Fig. 11 Crystallographic structure of 78 (left) and 77 (right). Top: molecular structure; bottom: packing mode (SO and SS intra and inter-
molecular interactions are represented by dotted lines) (from ref. 109).
Fig. 12 UV-Vis absorption spectra of alternated oligomers 79, 83 and
85 in CH2Cl2, from left to right (from ref. 109).
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developed, several groups began to investigate in more detail
the chemistry of EDOT or undertook the modification of
the chemical structure of the EDOT system itself in order to
manipulate its chemo-physical and electronic properties.
Hellberg and coworkers have recently reported a synthesis
of EDOT based on a novel one-step synthesis of 3,4-
dimethoxythiophene 89 by ring closure of 2,3-dimethoxy-1,3-
butadiene (Scheme 4).113 EDOT was then obtained by
transetherification of 89114 using ethylene glycol.113
EDOT and other 3,4-alkylenedioxy-thiophenes have been
synthesized by the double Mitsunobu reaction.115,116 Chiral
EDOT derivatives were obtained by the same method usingenantiomerically pure 1,2-propanediols.116
Pure chiral disubstituted EDOTs have been prepared by
transetherification of 3,4-dimethoxythiophene and electro-
polymerized into stereo- and regio-regular polymers.117
Probably one of the simplest modifications of the EDOT
structure involves the substitution of the ethylenedioxy bridge
in order to improve the solubility of the resulting polymer.
Thus, various examples of soluble polymers derived from
EDOT bearing alkyl, oligooxyethylene or alkylsulfonate
chains have been synthesized.15,19,20,42,43,47,118 As revealed by
spectroelectrochemical studies, the polymers derived from
alkyl-substituted EDOT or 3,4-propylenedioxythiophene
(ProDOT) show enhanced optical contrast in electrochromicdevices.20 On this basis, processable soluble polymers (9093)
have been recently developed around the ProDOT structure.119
Although the introduction of long alkyl chains represents
the simplest method to synthesize soluble conjugated poly-
mers. The mode of hybridization of the carbon serving as
anchoring point for the solubilizing group introduces a major
difference between poly(3-alkylthiophenes) (PATs) and the
polymers derived from alky-substituted EDOT and ProDOT.
For PATs, substitution of an sp2 carbon at the 3-position of
the thiophene cycle allows the side chain to remain coplanar
with the p-conjugated PT backbone. In contrast, for EDOT,
fixation of the alkyl chain at an sp3 carbon of the ethyl-
enedioxy bridge has two undesirable consequences. First, such
substitution creates a center of chirality thus giving rise to aconsiderable number of possible regio- and stereoisomers in
the resulting polymer. Second and more importantly, the fact
that the alkyl chain can no longer remain coplanar with the
p-conjugated system produces an increase of the distance
between the conjugated chains and hence an increase of the
band gap and a drop of the charge-carriers mobility.
A clear illustration of this effect is provided by the com-
parison of the UV-Vis spectra of a soluble polymer obtained
by oxidative chemical polymerization using FeCl3 of an EDOT
monomer derivatized with a decyl chain (94).
In chloroform solution, the spectrum of poly(94) exhibits
a well resolved fine structure with a lmax at 595 nm and a
00 transition at 654 nm (Fig. 13). Surprisingly, when the
polymer is processed into a solid film the optical spectrum
remains practically identical with however a small (ca. 5 nm)
Scheme 4 Synthesis of 3,4-dimethoxythiophene from 2,3-dimethoxy-
1,3-butadiene.
Fig. 13 UV-Vis absorption spectra of poly(94). Thin line in CH2Cl2,
thick line film spin-coated on glass (from ref. 120).
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hypsochromic shift of the absorption maxima.120 In the case of
poly(alkylthiophenes) the same experiment leads to a red shift
of the absorption maximum from 430440 nm in solution to
ca. 500 nm in the solid state due to the combined effects of
planarization and strong p-stacking interactions between the
conjugated chains in the aggregated phase.13 The absence of
such effects for alkyl-substituted PEDOT shows that the large
interchain distances imposed by the substituent attached at ansp3 carbon leads to a considerable decrease of p-stacking
interactions in the solid-state. As already discussed the
suppression of these interactions significantly contributes to
increase the band gap of the polymers.58,84
A possible solution to this problem consists of the
modification of the EDOT structure in order to attach the
solubilizing side chain at an sp2 carbon. To this end, we and
others have synthesized 3,4-phenylenedioxythiophene
(PheDOT) (95).121123
In order to obtain soluble polymer compounds, 96 and 97
were synthesized by transetherification of 3,4-dimethoxy-
thiophene using the appropriate catechols.122 Although
electropolymerization could be achieved, it was considerably
more difficult than that of conventional EDOT derivatives. In
fact, as indicated by high scan rate cyclic voltammetry,
replacement of the ethylenedioxy bridge by with a phenyl-
enedioxy moeity leads to a strong stabilization of the cationradical. As shown by ab initio computations at the hybrid
density functional theory level, the HOMO level of PheDOT is
slightly higher than that of EDOT. However whereas the
SOMO of the EDOT radical has high coefficients on the 2,5-
positions, in agreement with its straightforward electropoly-
merization, for the PheDOT cation radical SOMO coefficients
are essentially localized on the dioxin ring and null on the
2,5-positions of the thiophene ring (Fig. 14). These results are
in full agreement with the experiment showing that the high
stability of the PheDOT cation radical is not compatible with
efficient polymerization.122
Despite its difficult electropolymerization PheDOT repre-
sents an interesting platform for the development of new
classes of p-conjugated systems in particular oligomers, in
which the strong donor properties of EDOT analogues will be
associated with a solubilization by substitution of sp2 carbons
compatible with compact p-stacked organization in the solidstate.
3,4-ethylenedioxypyrrole (96) can be viewed as another deep
modification of the EDOT system. Whereas the monomer
shows a lower oxidation potential than EDOT, the resulting
polymer presents a larger band gap and a lower conduc-
tivity.20,124 Cava and coworkers have described the multistep
synthesis of 3,4-ethylenedioxyselenophene (97).125 The cyclic
voltammogram showed that this compound oxidizes at a
potential 0.26 V lower than that of EDOT under the same
experimental conditions. The CV of the polymer exhibits a
broad redox system extending from 21.0 to +1.0 V vs. SCE,
while an acetonitrile solution of the neutral polymer prepared
chemically using FeCl3 as oxidant shows an absorption maxi-mum at 594 nm.125
The polymerization of the disulfur analog of EDOT, namely
ethylenedithiathiophene (98), was reported by Kanatzidis and
coworkers in 1995.126 Although this compound oxidizes at a
potential 0.18 V lower than that of EDOT, the resulting
polymer shows a much higher oxidation potential and larger
band gap than PEDOT. This shortening of the effectiveconjugation length can be attributed to the distortion imposed
on the conjugated backbone by the steric interactions between
adjacent monomers.
As an intermediate case, we have synthesized thieno[3,4-b]-
1,4-oxathiane (99), in which one of the oxygen atoms of EDOT
has been replaced by sulfur.127 This compound could be
straightforwardly electropolymerized into a stable polymer
and, as expected, the electrochemical and optical properties
of the resulting polymer were intermediate between those of
PEDOT and of poly(98). Thus, the anodic peak potential was
found at +0.40 V vs. Ag/AgCl and the absorption maximum of
the undoped polymer (532 nm) was between that of PEDOT
(590 nm) and poly(98) (448 nm). A particularly interesting
property of compound 99 is that the difference in the electronic
effect of alkoxy and alkylsulfanyl groups introduces a dis-
symmetry in the electronic density at the 2 and 5 positions of
the thiophene ring, thus inducing a difference in reactivity
useful for regioselective substitution.127
Conclusion
Almost 15 years after its synthesis, PEDOT occupies a
prominent position among conducting polymers due, among
other things, to the multiple well-established technological
applications of its various conducting forms. On the other
Fig. 14 SOMO of the cation radicals, Left: EDOT, Right: PheDOT
(95). (From ref. 122, reproduced by permission of The Royal Society of
Chemistry.)
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hand, the prevention of undesired ab9 couplings, the large
decrease of the oxidation potential and the preservation of a
high reactivity at the terminal a-positions represent decisive
advantages which have been widely used for the synthesis of
electrogenerated functional conducting polymers as electrode
materials. Whereas direct substitution of EDOT presents only
limited advantages over 3-substituted thiophenes in terms of
polymerization potential, the incorporation of the EDOT unitin the structure of precursors of electrogenerated conducting
polymers represents a very efficient approach which has led to
the development of a huge number of functional polymers with
a wide scope of potential applications.
While many of these polymers have been synthesized from
tricyclic precursor structures with a functional median group
inserted between two lateral EDOT groups, recent work
has shown that the association of EDOTthiophene based
precursors, multi-site approaches and the application of
thiolate or alcoolate chemistry for functionalization allows
the synthesis of stable electroactive polymers derivatized with
functional groups sometimes difficult to incorporate in electro-
generated p-conjugated polymers.One of the most salient features of the recent chemistry
of EDOT concerns its progressive emergence as a unique
building block for the synthesis of different classes of
molecular functional p-conjugated systems. The discovery
that, in addition to a strong electron donor effect, EDOT
gives rise to self-rigidification of linearly p-conjugated
structures by means of intramolecular non-covalent interac-
tions between oxygen, sulfur and eventually other hetero-
atoms, undoubtely represents an important result for the
synthetic chemistry of functional p-conjugated systems. In
recent years, this self-structuring effect has been successfully
used for the optimization of the (opto)electronic properties
of various classes of molecular functional p-conjugatedsystems.
The synthesis of monodisperse extended conjugated oligo-
mers represents one of the most recent developments of the
EDOT chemistry. As shown by recent work, in this case too
self-structuration plays a major role leading to a significant
enhancement of the effective conjugation. On the other hand,
the strong electron donor effects of the EDOT unit, which
constitute a major tool for the modulation of the electronic
properties of extended oligomers, also render the analysis of the
relationships between the molecular structure of the oligomer
and the structure and electronic properties of the resulting
molecular material considerably more complex. Although the
realization of the first example of a field-effect transistorbased on an hybrid EDOT-based conjugated oligomer
illustrates the potentiality of this class of oligomers as organic
semi-conductors, this preliminary result confirms the need
to concentrate much research effort on the elucidation of
the structureproperty relationships in these new classes of
conjugated oligomers.
Solubilization represents another specific problem posed
by the structure of EDOT. While phenylenedioxythiophene
represents a first attempt in that direction, it is clear that
further work is needed to develop soluble EDOT-based con-
jugated systems compatible with compact p-stacking interac-
tions in the solid state.
The modification of the chemical structure of EDOT itself,
by replacement of some of its constitutive atoms, is another
quite recent topic which, beyond its immediate fundamental
interest, could also lead to major advances in the future. Here
also, intense effort to develop creative synthetic chemistry
seems more than ever necessary.
AcknowledgementsThe authors wish to thank their co-workers, post-doctoral
fellows and PhD students named in some of the cited
references for their invaluable contribution to some of the
work covered in this review.
Jean Roncali,* Philippe Blanchard and Pierre FrereGroupe Systemes Conjugues Lineaires, CIMMA, UMR CNRS 6200,Universite dAngers, 2 Bd Lavoisier, Angers, France.E-mail: [email protected]
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