The coupling of substituted carbazole compounds through carbon-carbon bond formation upon one-electron oxidation is shown to be a highly versatile approach to the formation of redox polymer films. Although the polymerization of single carbazole units has been proposed earlier, we show that by tethering pairs of carbazoles double sequential dimerization allows for facile formation of redox polymer films with fine control over film thickness. We show that the design of the monomers and in particular the bridging units is key to polymer formation, with the diaminobenzene motif proving advantageous, in terms of the matching to the redox potentials of the monomer and polymer film and thereby avoiding limitations in film thickness (autoinsulation), but introduces unacceptable instability due to the intrinsic redox activity of this moiety. The use of a diimide protecting group both avoids complications due to p-diamino-benzene redox chemistry and provides for a redox polymer in which the photoluminescence of the bis-carbazole moiety can be switched reversibly (on/off) with redox control. The monomer design approach is versatile enabling facile incorporation of additional functional units, such as naphthalene. Here we show that a multicomponent carbazole/naphthalene containing monomer (APCNDI) can form redox polymer films showing both p- and n- conductivity under ambient conditions and allows access to five distinct redox states, and a complex electrochromic response covering the whole of the UV/vis-NIR spectral region. The highly effective quenching of the photoluminescence of both components in poly-APCNDI enables detailed characterization of the redox polymer films. The poly-APCNDI films show extensive charge trapping, which can be read out spectroscopically in the case of films and is characterized as kinetic rather than chemical in origin on the basis of UV/vis-NIR absorption and resonance Raman spectroscopic analyses. The strong resonantly enhanced Raman scattering for the various oxidized and reduced states of APCNDI enables nondestructive "read-out" of the state of the polymer, including that in which charges are trapped kinetically at the surface, making poly-APCNDI highly suitable for application as a component in organic nonvolatile memory devices.
The coupling of substituted carbazolecompounds through carbon-carbon bond formation upon one-electron oxidation is shown to be a highly versatile approach to the formation of redox polymer films. Although the polymerization of single carbazole units has been proposed earlier, we show that by tethering pairs of carbazoles double sequential dimerization allows for facile formation of redox polymer films with fine control over film thickness. We show that the design of the monomers and in particular the bridging units is key to polymer formation, with the diaminobenzene motif proving advantageous, in terms of the matching to the redox potentials of the monomer and polymer film and thereby avoiding limitations in film thickness (autoinsulation), but introduces unacceptable instability due to the intrinsic redox activity of this moiety. The use of a diimide protecting group both avoids complications due to p-diamino-benzene redox chemistry and provides for a redox polymer in which the photoluminescence of the bis-carbazole moiety can be switched reversibly (on/off) with redox control. The monomer design approach is versatile enabling facile incorporation of additional functional units, such as naphthalene. Here we show that a multicomponent carbazole/naphthalenecontaining monomer (APCNDI) can form redox polymer films showing both p- and n- conductivity under ambient conditions and allows access to five distinct redox states, and a complex electrochromic response covering the whole of the UV/vis-NIR spectral region. The highly effective quenching of the photoluminescence of both components in poly-APCNDI enables detailed characterization of the redox polymer films. The poly-APCNDI films show extensive charge trapping, which can be read out spectroscopically in the case of films and is characterized as kinetic rather than chemical in origin on the basis of UV/vis-NIR absorption and resonance Raman spectroscopic analyses. The strong resonantly enhanced Raman scattering for the various oxidized and reduced states of APCNDI enables nondestructive "read-out" of the state of the polymer, including that in which charges are trapped kinetically at the surface, making poly-APCNDI highly suitable for application as a component in organic nonvolatile memory devices.
Smart (stimuli responsive)
surfaces[1] are attracting increasing attention,[2−4] not least in the field
of molecular electronics,[5] due to the opportunities
presented by redox switching in rapid localized control of physical
and optical properties. Electrochromism, the inducing of reversible
color changes by application of a voltage, was first observed in inorganic
semiconductors.[6] The later discovery of
organicconducting and redox polymers has enabled fine control of
HOMO–LUMO band-gaps and hence optical properties as well as
their facile processing and application to foldable devices. D–A–D
(donor–acceptor–donor) oligoimides in particular have
seen application already in high-performance nonvolatile memory devices,[7−16] logic gates,[17] and nonlinear optical
materials.[18,19] Intra- and intermolecular interactions
in such multicomponent systems often alter the functionality of their
individual components,[20,21] which can provide opportunities
in their application.Carbazole and its derivatives have been widely studied for their
various physical and electronic properties, the most studied of which,
poly(N-vinylcarbazole), was the first nitrogen heterocycle
containing polymer to show hole transport properties.[22] The discovery of the optical and electrical properties
of carbazolecontaining polymers and oligomers has stimulated their
application in areas as diverse as organic light emitting diodes (OLEDs)
and organic-thin film transistors,[23−25] organic solar cells,[26−28] and sensors.[29]Carbazole is often
modified with a moiety to allow for incorporation
in a polymer, e.g., with vinyl groups[30,31] or through
Suzuki coupling,[32] since although the ability
of N-substituted carbazoles to undergo polymerization has been proposed,
Karon and Lapkowski concluded, in their recent review, that oxidation
of N-substituted carbazoles leads mainly to dimers as a consequence
of charge delocalization in the 3–3′ dimer.[33] Indeed, Siove and co-workers showed that a monomer
in which two carbazole units are tethered by an N-substituted alkyl
spacer merely leads to sequential dimerization upon chemical oxidation
to form a polymer thatcould be spin-cast on electrodes.[34] The C–Ccoupling para to the nitrogen
upon (electro)oxidation[24−26] via a 4 electron ECCE process
is analogous to the dimerization of indoline derivatives[35] and N,N-dialkyl
substituted anilines,[36−38] which occur readily. Moreover, direct coupling of
two of such moieties covalently via the amine group results in chain-growth
elongation of the bisindoline scaffold (Scheme ) with each unit coupling to another molecule.[39]
Scheme 1
ECCE Mechanism for Sequential Dimerization
of Alkyl N,N-Coupled Bisindolines
and Related Compounds[34,39]
Koyuncu et al. reported a carbazolecoupled to either
perylene[40] or naphthalimide[41] to form energy donor/acceptor (D–A) systems,
which can be
immobilized by electrochemical coupling of the carbazole units. The
films formed show moderate quenching of the fluorescence of both donor
and acceptor in the dyads but almost complete quenching of photoluminescence
in the films formed electrochemically (Figure ). The use of only a single carbazole unit
in this system, however, requires that each carbazole unit couples
to two others in order to form a polymer backbone with pendent naphtal-
and perylene-imide units. However, the steric overcrowding expected
in the system reported by Koyuncu et al., the stability of the initially
formed bis-carbazole dication (which is present at the potentials
required for oxidation of monomer), and the poor mechanical stability
of the films formed, indicate that dimerization rather than polymerization
occurred, with insolubility being the primary driving force for immobilization
on the electrodes used. The choice of spacer unit between the carbazole
and perylene/naphtalimide (Scheme ) has a pronounced effect on the efficiency of carbazole–carbazolecoupling and the final structure of the films formed.
Figure 1
Approaches toward carbazole
and naphthalene derived Donor–Acceptor
(polymer) systems.
Approaches toward carbazole
and naphthalene derived Donor–Acceptor
(polymer) systems.The spacer unit, in such
systems, plays an important role in determining
the overall function of the systems. Earlier studies on compounds
in which a functional unit, such as a dithienylethene photochromic
switch, was tethered to a pair of electrodimerizable/polymerizable
units showed that the introduction of a phenyl spacer aids the polymerization
process and improves the retention of the functionality of the photoswitchable
moiety.[42−44] Koyuncu et al. took a similar approach in which carbazole
units are attached directly at their 3-position to both ends of a
naphthalene diimide, enabling polymerization through sequential dimerization
(Figure ).[32] With this approach, however, only partial quenching
of photoluminescence was observed, ascribed in part due to perturbation
of the properties of the carbazole by direct attachment of the diimide
unit to it.1,4,5,8-Naphtalene diimides (NDIs) are chemically
robust chromophores
which have seen widespread application over the last decades in supramolecular
systems such as rotaxanes,[45,46] catenanes,[47,48] nanotubes,[49] ion channels,[50] foldamers,[51] and
synthetic photosystems.[52] Their tendency
to self-organize both at the solid state and in solution due to their
planarity and to engage in ππ stacking has made them appealing
to supramolecular chemistry as they can form or be incorporated readily
within supramolecular assemblies. Furthermore, the electronic properties
of NDI have found application in sensing and in multicomponent systems
in which energy and electron transfer processes are utilized. For
example, Takenaka et al. have employed an NDI bearing redox-active
ferrocenyl moieties to discriminate between double stranded DNA and
single stranded DNA electrochemically.[53] The radical monoanionic form of NDI is readily accessible by chemical
and electrochemical reduction,[54] and its
electron deficiency in its neutral state favors interaction with electron
rich species and anions as highlighted elegantly by Matile et al.
in their study of charge transfer (anion-π interactions) and
transport between substituted NDI monomers and nanorods with a variety
of anions.[55] More recently, Saha et al.
reported light-gated electron transfer from anions to aryl substituted
NDI.[56,57]The wider range of applications thatcan be realized makes the
combination of carbazole and NDI in an electrochromicpolymer film
highly appealing.[58,59] Several approaches toward this
goal have been reported to date, making use of various carbazole structures
and naphthalene derivatives (Figure ). Kozycz and co-workers observed quenching of the
emission at 700 nm in a D–A carbazole–naphthaleneimidepolymer obtained through chemical coupling.[60] A drawback of the latter approach is the synthetic effort of chemical
coupling, as well as the risk of presence of residual palladium, which
limits the range of applications. Lav et al. utilized the propensity
of tethered carbazoles to dimerize, forming numerous cross-links through
sequential electrodimerization in an oligomer containing carbazole
side chains.[61] The key challenge in forming
robust redox polymers based on the combination of NDI and carbazole
is to achieve polymerization rather than dimerization and to avoid
other electrochemically induced reactions.Here, we report the
synthesis and characterization of amino-phenyl
carbazolecyclohexane diimide (APCCDI), Figure , and its oxidative electropolymerization
on a range of electrode materials under ambient conditions, i.e.,
without need for strong Lewis acids or inert conditions. The optical
and electrochemical properties of the monomer and redox-active polymer
films are characterized by UV/vis, FTIR and emission spectroscopy,
and cyclic voltammetry.
Figure 2
Structure of amino-phenyl carbazole (APC), cyclohexane
dianhydride (CDA), and amino-phenyl carbazole cyclohexane
diimide (APCCDI), naphthalene dianhydride (NDA), and amino-phenyl carbazole naphthalene diimide (APCNDI).
Structure of amino-phenyl carbazole (APC), cyclohexane
dianhydride (CDA), and amino-phenyl carbazolecyclohexane
diimide (APCCDI), naphthalene dianhydride (NDA), and amino-phenyl carbazole naphthalene diimide (APCNDI).In addition, two carbazolecompounds
were prepared for modeling
of the oxidative coupling and the impact of the functional groups
present in the multicomponent systems on electrochemical stability
(Figure and Scheme ). We show that while
the diimide unit performs well under electrochemical conditions, the
use of a simpler N-aryl amide linkage D1 shows instability due to the quinoidal character of the oxidized p-diamino linker, with decomposition competing with carbazole-carbazolecoupling.
Figure 3
Model compounds used to study carbazole oxidative dimerization, N-(p-carbazole phenyl)acetamide (D1), and methyl p-carbazole benzoate (D2), amino-phenyl carbazole cyclohexane imide (A1), amino-phenyl carbazole cyclohexane imide (I1), and
its dimer obtained by chemical oxidation (I2).
Scheme 2
One Electron Oxidation of Bis-Aminophenyl Modified
Carbazole is Centered
on the Carbazole Unit but is Expected to Have Significant Contribution
from Resonance Structures Involving the Protected Bis-Aminophenyl
Unit, Exposing It to Competing Hydrolysis Reactions
Model compounds used to study carbazole oxidative dimerization, N-(p-carbazole phenyl)acetamide (D1), and methyl p-carbazole benzoate (D2), amino-phenyl carbazole cyclohexane imide (A1), amino-phenyl carbazole cyclohexane imide (I1), and
its dimer obtained by chemical oxidation (I2).Model compounds such as the benzoate
based D2, however,
showed the expected spectroscopic properties of the carbazole dimers
after oxidative electrolysis, with a slight red-shift in both the
UV/vis absorption and fluorescence spectra. The model monomer (I1) and dimer (I2) of APCCDI, with
a single instead of double diimide, provide insight into its properties
in the monomeric and polymeric form.The electrochemical performance
of the phenyl carbazole unit, linked
through an imide (i.e., as in APCCDI), was built upon
in a more complex system in which an NDI unit is coupled via imides
to two carbazole units to form APCNDI (Figure ) and access the reductive
electrochemistry and symmetric rigid structure of NDI in multifunctional
polymer films. We show thatcomplete quenching of the photoluminescence
of both NDI and bis-carbazole is achieved, which enables the study
of the polymer films formed, and assignment of charge trapping as
kinetic or thermodynamic (vide infra), using multiwavelength resonance
Raman microspectroscopy under electrochemical control. The APCNDIpolymer films formed show reductive and oxidative electrochromism
and selective enhancement of Raman bands of the various accessible
redox states. We show that oxidative and reductive kineticcharge
trapping can be achieved in thicker films and can be “read
out” in poly-APCNDI by resonance
Raman spectroscopy nondestructively, providing for applications in
nonvolatile memory.
Experimental Section
Materials
Reagent
grade carbazole, p-bromonitrobenzene, copper iodide,
1,10-phenantroline, potassium
carbonate, hydrazine monohydrate, pyridine, acetic anhydride, cesium
carbonate, palladium on charcoal, tetrabutyl ammonium hexafluorophosphate
(TBAPF6), FeCl3, 4-iodoaniline, 4-iodobenzoic
acid, Cu2O, and 1,4,5,8-naphthalenetetracarboxylic dianhydride
were purchased from Sigma-Aldrich and were used as-received. Reagent
grade 1,2-cyclohexane anhydride and 1,2,4,5-cyclohexane dianhyride
were purchased from TCI Co., Ltd. and used as-received. Amino-phenyl
carbazole (APC) was stored as its HCl salt (Supporting Information, SI), and liberated before
use. Compound D1 is the precursor to the APC·HCl salt. Compound D2 was synthesized through
esterification of p-iodobenzoic acid followed by
cuprous oxide mediated carbazolecoupling (SI). Details of the synthesis and characterization of APCCDI and APCNDI are provided as SI (Figures S1–S18).UV/vis
absorption spectroscopy, electrochemistry, in situ UV/vis absorption,
and resonance Raman spectroelectrochemical experiments were conducted
in spectroscopic (UVASOL) grade dichloromethane (Merck).
Physical Methods
1HNMR and 13CNMR spectra were obtained
on a Varian Mercury Plus 399.93 MHz spectrometer.
Chemical shifts are reported in ppm (δ), coupling constants
in Hz, multiplicity is noted as follows: s = singlet, d = doublet,
t = triplet, m = multiplet. Chemical shifts are with respect to tetramethylsilane
and referenced to residual solvent (either CHCl3 or DMSO-d5) signals. UV/vis absorption spectra were recorded
on an Analytik Jena Specord 600 in concentrations ranging from 30
to 60 μM in dichloromethane. In situ UV/vis and vis–NIR
absorption spectra, obtained using a quartz cuvette as electrochemical
cell with a poly-APCNDI modified ITO working electrode,
were recorded on an Analytik Jena Specord 600 and a JASCO FT/IR-4600,
respectively. Spectra were referenced to a bare ITO coated glass slide
in 0.1 M TBAPF6 in dichloromethane and solutions with and
without APCNDI-monomer were exchanged by syringe to maintain
the consistency of the optical path. Electrochemical data were obtained
using a CHI760B electrochemical workstation (CH Instruments), all
potentials are quoted with respect to the SCE and a sweep rate of
0.1 V s–1 was employed unless stated otherwise.
A three electrode arrangement was employed with a glassy carbon (diameter
3 mm), platinum (diameter 1.5 mm), or gold (dia 1.5 mm) disc working
electrode, a Ag/AgCl wire reference and a platinum wire counter electrode,
under argon purge when scanning to negative potentials (<−0.2
V vs SCE). For bulk electrolysis, a rectangular reticulated vitreous
carbon (RVC) electrode from ERG Materials & Aerospace Corporation,
Oakland, CA, was employed as working electrode. Emission spectra were
obtained using a Andor Newton 970-BV EMCCD (operated in CCD mode)
camera mounted to a shamrock163 spectrograph with a 300 l/mm grating
blazed at 300 nm fiber coupled to a THORLABS cuvette holder (for solutions)
or a Nikon TE-Eclipse inverted microscope for modified electrodes.
Excitation at 300 and 365 nm used Fiber coupled LEDs (thorlabs). FTIR
spectra were recorded on a PerkinElmer FTIR Spectrum 400 equipped
with a UATR attachment. Mass spectra were recorded on a MALDI TOF
Voyager DE-Pro by Applied Biosystems and a Xevo G2 Q-TOF DART by Waters
Corporation. In situ Resonance Raman spectroelectrochemistry was performed
following electropolymerization on a platinum disc working electrode
by repeated cyclic voltammetry, followed by washing of the polymer
modified electrode with dichloromethane and immersion in dichloromethane
with 0.1 M TBAPF6. In situ measurements were performed
on a PerkinElmer Raman station with excitation at 785 nm using a quartz
cuvette as electrochemical cell. Raman spectra were recorded at λexc 266 nm (0.6 mW at sample, obtained by frequency doubling
of the 532 nm output of a DPSS laser using a Newport WaveTrain) and
355 nm (10 mW at sample, Cobolt lasers) in 135° and 180°
backscattering mode, respectively. Raman scattering was collimated
and subsequently refocused by a pair of 25 mm planoconvex lens (7.5
and 15 mm focal lengths, respectively) into a Shamrock500 spectrograph
(Andor technology) with a 2400 l/mm grating blazed at 300 nm onto
a iDus-420-BU2 CCD (Andor Technology). Spectra were acquired and processed
using Andor Solis and PerkinElmer Spectrum 10.0, respectively. Fluorescence
spectra were recorded using quartz cuvettes containing 5 nM solutions
of analyte in dicholoromethane with excitation provided by a 75 W
xenon lamp coupled to a Zolix 150 mm monochromator and to a qpod (Quantum
Northwest) temperature controlled cuvette holder. The emission was
collected at 90° through a fiber opticconnected to an iDus-420-OE
CCD camera (Andor Techology).
Results and Discussion
UV/vis
Absorbance and Emission Spectroscopy of D1 and D2
Although
the polymerization of carbazole derivatives has been proposed
elsewhere,[62,63] the propensity of N-phenyl carbazole derivatives to undergo oxidative C–C bond
formation to form dimers rather than other electrochemical reactions[33] was investigated in the model compounds D1 and compound D2 (Figure ). Both D1 and D2 are comprised of an aryl N-substituted carbazole unit, however, D2 does not bear the p-bis-amino motif of D1. Although the cyclic voltammetry of D1 (Figure S6) indicates a propensity to undergo
dimerization by C–Ccoupling of the carbazole units, preparative
electrolysis resulted in a general decrease in UV absorbance and completely
loss in emission intensity (Figure upper). In contrast, cyclic voltammetry (Figure S7) and preparative oxidative electrolysis
of solutions of D2 resulted in a minor broadening in
the UV/vis absorbance spectrum and a red shift of the emission spectrum
consistent with formation of a bis-carbazole (Figure lower). In both
cases, there was no indication of formation of polymer films at the
working electrodes. The greater stability, with regard to oxidation,
of D2 indicates that for D1 the quinoidal
character of the p-bis-amino motif is important and
reaction of this moiety after oxidation may compete effectively with
carbazole dimerization.
Figure 4
(Top left) UV/vis absorbance and (top right,
λexc 300 nm) emission spectra of D1 before
(black) and after
preparative anodic electrolysis (black dotted) at 1.2 V for 15 min.
(Bottom left) UV/vis absorbance and (bottom right, λexc 300 nm) emission spectra of D2 in dichloromethane (solid
line) before and after preparative anodic electrolysis (dotted line)
at 1.2 V for 1 h. (Bottom right) Emission spectra showing change in
relative emission intensity and normalized spectra. Conditions: in
dichloromethane with 0.1 M TBAPF6 with a carbon mesh working,
SCE reference and platinum counter electrode.
(Top left) UV/vis absorbance and (top right,
λexc 300 nm) emission spectra of D1 before
(black) and after
preparative anodic electrolysis (black dotted) at 1.2 V for 15 min.
(Bottom left) UV/vis absorbance and (bottom right, λexc 300 nm) emission spectra of D2 in dichloromethane (solid
line) before and after preparative anodic electrolysis (dotted line)
at 1.2 V for 1 h. (Bottom right) Emission spectra showing change in
relative emission intensity and normalized spectra. Conditions: in
dichloromethane with 0.1 M TBAPF6 with a carbon mesh working,
SCE reference and platinumcounter electrode.Compound I1, prepared from APC (aminophenyl
carbazole) by reaction with cyclohexyl-1,2-dicarboxy anhydride was
dimerized by chemical oxidation[64,65] to yield model compound I2. Dimerization of I1 to form I2 results in broadening of the UV absorption bands and a redshift
in the emission (Figure ), as observed for D1/D2.
Figure 5
Synthesis of I1 and I2 from the APC·HCl salt and
(left) UV/vis absorbance and (right)
emission spectra of I1 (solid line) and I2 (dotted line) in dichloromethane.
Synthesis of I1 and I2 from the APC·HCl salt and
(left) UV/vis absorbance and (right)
emission spectra of I1 (solid line) and I2 (dotted line) in dichloromethane.The retention of the absorption and emission properties upon
oxidative
coupling of I1 to form I2 indicates that
the diimideconnection prevents involvement of the p-bis-amino motif in the redox chemistry of the compounds. Hence the
structure APCCDI, prepared analogously to I1 (see SI), was expected to undergo sequential
oxidative dimerization of the imide-linked phenyl carbazoles (Scheme ).Indeed the
cyclic voltammetry of APCCDI is as expected
for an indolecontaining compound,[35−37] i.e., a 4-electron ECCE
process resulting in dimerization via aryl–aryl coupling (Figure ). Two carbazole
radical cations, formed an electrochemically, couple and undergo double
deprotonation to rearomatize. This process is followed by immediate
oxidation to the product’s doubly cationic state at the applied
potential, with two new redox waves on the return cycle assigned to
the first and second reductions of the [bis-carbazole]2+ units formed.
Figure 6
Oxidative cyclic voltammetry of APCCDI (0.1
mM) in
dichloromethane (SCE reference and platinum counter electrode, 0.1
M TBAPF6, scan rate 0.1 V s–1) at a Au
working electrode (d = 3 mm), and the corresponding
mechanism of the electrochemical dimerization. Initial cycle (thick
line), second cycle (dotted line).
Oxidative cyclic voltammetry of APCCDI (0.1
mM) in
dichloromethane (SCE reference and platinumcounter electrode, 0.1
M TBAPF6, scan rate 0.1 V s–1) at a Au
working electrode (d = 3 mm), and the corresponding
mechanism of the electrochemical dimerization. Initial cycle (thick
line), second cycle (dotted line).In contrast to compound I1, however, dimerization
leaves two carbazole units connected via the diimide bridges, which
can undergo subsequent coupling to other carbazole units and hence
stepwise chain elongation. The oligomers are insoluble and deposit
on the electrode surface readily leading to the buildup of a redox
polymer manifested in the steady increase in current (Ip,a and Ip,c) of the redox
waves of the bis-carbazole unit (Figure ). Importantly the oxidation potential of APCCDI is close to that of the second oxidation of the bis-carbazole
unit formed and hence film growth is not limited by lack of conductivity
at the onset potential for polymerization. The voltammetry of polymer
modified electrode in monomer free solution shows the redox waves
of poly-APCCDI, indicating that the polymer is well adhered
to the electrode surface and is not affected substantially by the
presence adventitious water or oxygen. Films from poly-APCCDI were formed readily at glassy carbon, platinum, and ITO on glass
slide electrodes indicating that surface polymer interactions are
not especially important in achieving adhesion, but instead that solubility
is the primary driving force.
Figure 7
(Left) Cyclic voltammetry of APCCDI (0.1 mM) at a
Au electrode (d = 3 mm), and (right) cyclic voltammetry
of the poly-APCCDI modified electrode in a monomer free
solution. In dichloromethane, 0.1 M TBAPF6, Pt counter,
and SCE working electrode, scan rate 0.1 V s–1),
final surface coverage is estimated to be 2.4 × 10–8 mol cm–2 on the basis of the anodic charge passed.
(Left) Cyclic voltammetry of APCCDI (0.1 mM) at a
Au electrode (d = 3 mm), and (right) cyclic voltammetry
of the poly-APCCDI modified electrode in a monomer free
solution. In dichloromethane, 0.1 M TBAPF6, Ptcounter,
and SCE working electrode, scan rate 0.1 V s–1),
final surface coverage is estimated to be 2.4 × 10–8 mol cm–2 on the basis of the anodiccharge passed.
Electrochemical Modulation
of poly-APCCDI Fluorescence
The fluorescence of poly-APCCDI was expected to be similar
to that of I2, however, immobilization in a polymer film
at a, e.g., Au, macroelectrode could result in emission quenching
due to intermolecular interactions. The emission of poly-APCCDI, excited at λexc 365 nm, was less well-defined
(broader) than that of I2, but is nevertheless, together
with its slight red-shift, typical for the bis-carbazole motif.[66] Oxidation resulted in complete quenching of
photoluminescence with full recovery upon reduction to the neutral
state (Figure ). Monitoring
of photoluminescence switching during multiple potential steps shows
that relatively rapid switching on and off of polymer emission with
a response time that indicated charge diffusion was limiting (vide
infra).
Figure 8
(upper left) In situ photoluminescence (λexc =
365 nm) of poly-APCCDI and (upper right) the corresponding
cyclic voltammetry of the poly-APCCDI modified Au electrode
in dichloromethane (0.1 V s–1, 0.1 M TBAPF6). Multistep potential switching cycles with alternating polarization
at 0 V for 30 s and 1 V for 15 s. (lower left) current response upon
switching the potential and (lower right) the corresponding photoluminescence
at 520 nm (λexc 365 nm). SCE reference and platinum
counter electrodes.
(upper left) In situ photoluminescence (λexc =
365 nm) of poly-APCCDI and (upper right) the corresponding
cyclic voltammetry of the poly-APCCDI modified Au electrode
in dichloromethane (0.1 V s–1, 0.1 M TBAPF6). Multistep potential switching cycles with alternating polarization
at 0 V for 30 s and 1 V for 15 s. (lower left) current response upon
switching the potential and (lower right) the corresponding photoluminescence
at 520 nm (λexc 365 nm). SCE reference and platinumcounter electrodes.
Multiresponsive Bis-Carbazole
Based Redox Polymer Films Incorporating
Naphthalene Diimide
The versatility of the bis-imide bridging
motif in APCCDI, prompted the incorporation of a naphthalene
unit to increase functionality and the preparation of APCNDI (for details of synthesis and characterization, see SI, and Figure S16). The absorption spectrum of APCNDI shows the characteristic
vibronic progression (π–π* transition) of the naphthalenediimide with maxima at 320, 340, 360, and 380 nm, which overlap with
the lowest π–π* transitions of the carbazole moiety
(Figure ). The absorption
bands are shifted bathochromically compared with the precursor 1,4,5,8-naphthalenetetracarboxylic
dianhydride (NDA).[54] At λexc 266 nm, the emission spectrum of an equimolar mixture of NDA and p-CMBz is dominated by carbazole emission (Figure ),[67,68] consistent with the large difference in molar absorptivity of the
components. At λexc 355 nm, the emission from both
components is similar in intensity. In contrast, the APCNDI shows essentially no emission upon excitation at either wavelength
with only Raman scattering from solvent observed, indicating highly
efficient emission quenching, considering the components redox chemistry
(vide infra), by photoinduced electron transfer (PET) from the carbazole
to the naphthalene moieties (Scheme ). Importantly, the extent of quenching seen in these
data confirm the absence of unreacted NDA and the carbazole precursor
in APCNDI and contrasts sharply with that observed for
the naphthalene bis-carbazole system reported by Koyuncu, in which
emission was observed and even increased 3-fold with subsequent electropolymerization.[32]
Figure 9
(Top) UV/vis absorption spectra of APCNDI (black),
(p-carbazole)methyl benzoate (dotted line) and 1,4,5,8-naphthalenetetracarboxylic
dianhydride (dashed line) and (bottom) emission spectra of equimolar
solutions of 1,4,5,8-naphthalenetetracarboxylic dianhydride (NDA), (p-carbazole)methyl benzoate aminophenylcarbazole
(p-CMbz), a 50/50 mixture of the NDA and p-CMBz, and APCNDI. Excitation at (left) 266 nm excites the carbazole unit selectively,
while (right) at 355 nm both the p-CMBz and NDA components are excited.
Scheme 3
Photo-Induced Electron Transfer from a Carbazole (Cbz) Donor
to a
Naphthalene Diimide (NDI) Acceptor
(Top) UV/vis absorption spectra of APCNDI (black),
(p-carbazole)methyl benzoate (dotted line) and 1,4,5,8-naphthalenetetracarboxylic
dianhydride (dashed line) and (bottom) emission spectra of equimolar
solutions of 1,4,5,8-naphthalenetetracarboxylic dianhydride (NDA), (p-carbazole)methyl benzoate aminophenylcarbazole
(p-CMbz), a 50/50 mixture of the NDA and p-CMBz, and APCNDI. Excitation at (left) 266 nm excites the carbazole unit selectively,
while (right) at 355 nm both the p-CMBz and NDAcomponents are excited.
Resonance Raman Spectroscopy of APCNDI
The strong blue
emission of both carbazole and naphthalene diimide precludes the application
of resonance Raman spectroscopy with excitation in the 250–400
nm range (vide supra and Figure S19). The
highly efficient photoinduced electron transfer quenching from the
carbazole to the NDI moiety observed in APCNDI, however,
allows resonance Raman spectra to be recorded in dilute solutions
at λexc 266 and 355 nm (Figure ). Enhancement of Raman bands at 1625 and
1237 cm–1 corresponding to those observed in the
Raman spectra of carbazole is seen at λexc 266 nm
and assigned to aromatic ring stretch and C–N stretch vibrations,
respectively, of the carbazole moiety only (since the NDI unit does
not absorb significantly at this wavelength and indeed NDA shows only
very weak resonance enhancement at λexc 266 nm, Figure S20). The carbazole in plane bending modes
at 1178 and 1019 cm–1, and out of plane bending
mode at 705 cm–1 were also observed. Resonance enhancement
of both the naphthalene diimide and carbazole moieties of APCNDI is observed at λexc 355 nm (Figure ). The bands at 1724 and 1685 cm–1 are assigned to naphthaleneC=O stretching, while the carbazoleC=C stretch is observed at 1627 cm–1 together
with bands at 1608 and 1415 cm–1 assigned as naphthalene
aromaticC=C and C–C stretching modes. Bands at 1111,
1073, and 1033 cm–1 are assigned to in-plane, and
713, 657, and 605 cm–1 to out-of-plane C–H
bending modes of APCNDI. The bands at 1569, 1386, 858,
823, and 537 cm–1 are useful in assignment of the
resonance Raman spectra of the polymer films formed (vide infra).
Figure 10
Resonance
Raman spectra (λexc (left) 266 nm and
(right) 355 nm) of APCNDI (i) in acetonitrile and (ii)
in dichloromethane. *Distortions due to imperfect subtraction of Raman
scattering of the solvent.
Resonance
Raman spectra (λexc (left) 266 nm and
(right) 355 nm) of APCNDI (i) in acetonitrile and (ii)
in dichloromethane. *Distortions due to imperfect subtraction of Raman
scattering of the solvent.
Cyclic Voltammetry of APCNDI
The redox chemistry of APCNDI between 0.0 and −1.7 V vs SCE is typical of
an NDI (naphthalene) moiety with two reversible redox processes at
−0.80 V and −1.20 V, with no evidence of polymer film
formation even with repeated cycling between 0.0 and −1.7 V
(Figure ). The redox
chemistry between 0.0 and 1.4 V vs SCE is identical to that of APCCDI, with efficient formation of a redox polymer film,
as expected with sequential coupling of each carbazole moiety to build
up a film of poly-APCNDI on the electrode. At a scan
rate of 0.1 V s–1, the cyclic voltammograms can
undergo 100 segments while showing a steady increase of the redox
response throughout. Although film thicknesses cannot be determined
precisely from the redox response, due to incomplete charge transfer
due to charge trapping (vide infra), an estimation can be made of
the upper and lower limits of surface coverage by comparing cathodic
and anodiccharge passed. The surface coverages determined under these
conditions are between 1.2 and 1.6 * 10–9 mol cm–2 at a glassy carbon electrode, which when compared
with typical monolayer coverages that are the range of 10–10 to 10–11 mol cm–2, indicates
ca. 10 to 15 monolayer equivalents.[69] Discharge
peaks are observed during cyclic voltammetry, in monomer containing
solution, typically after the third or fourth cycle and grow incrementally
thereafter. Surface coverage at this point is estimated to be between
1.5 and 1.8 × 10–10 mol cm–2, which is in the order of a one to two monolayers.
Figure 11
(Left) Reductive cyclic
voltammetry of poly-APCNDI and (center)
initial oxidative cyclic voltammetry of APCNDI (0.1 mM)
in dichloromethane (0.1 V s–1, 0.1 M TBAPF6, argon purged, GC working electrode, with iR compensation
applied) with assignment of redox processes.
(Right) Repeated oxidative cyclic voltammetry of APCNDI showing a steady increase in signal for poly-APCNDI. SCE reference and platinum counter electrodes.
(Left) Reductive cyclic
voltammetry of poly-APCNDI and (center)
initial oxidative cyclic voltammetry of APCNDI (0.1 mM)
in dichloromethane (0.1 V s–1, 0.1 M TBAPF6, argon purged, GC working electrode, with iR compensation
applied) with assignment of redox processes.
(Right) Repeated oxidative cyclic voltammetry of APCNDI showing a steady increase in signal for poly-APCNDI. SCE reference and platinumcounter electrodes.The redox response of the poly-APCNDI formed
on a
range of electrode types is retained upon washing and transferring
to monomer free solution (Figure ) and are stable under repeated cycling between 0.2
and 1.2 V, confirming the chemical and mechanical robustness of the
films, i.e., with regard to adventitious water and oxygen. Notably,
when performing cyclic voltammetry over the potential range of both
redox-active species, i.e., between −1.0 and 1.4 V, a prepeak
to either or both of the cathodic and anodic processes appears (Figure ). This occurrence
was assigned to charge trapping, the characterization of which will
be discussed below. A linear dependence of current of the main redox
waves on scan rate (up to 2 V s–1) is observed as
expected for a surface confined redox process (Figure S21).
Figure 12
(left) Cyclic voltammetry of a poly-APCNDI modified
platinum working electrode in monomer free dichloromethane (with 0.1
M TBAPF6).The anodic wave at 0.8 V is due to release of
trapped charges (vide infra) from reduction. Cathodic charge trapping,
present in complete overlap with the reduction at −0.6 V here,
is also observed clearly under monomer free conditions on an ITO working
electrode (Figure S22). (Right) Cyclic
voltammetry of a poly-APCNDI modified glassy carbon electrode
in monomer free dichloromethane. Initial scan toward negative potentials
from 0.0 V shows a reversible one electron redox wave (A) with a corresponding
discharge peak (B) on the return cycle toward positive potentials
which is absent on the second cycle in which the switching potential
is 0.3 V. The third consecutive cycle to positive and the negative
potentials shows a discharge peak due to trapped positive charges
(D) (with 0.1 M TBAPF6, platinum counter, and SCE reference
electrode, scan rate 0.1 V s–1). SCE reference and
platinum counter electrodes.
(left) Cyclic voltammetry of a poly-APCNDI modified
platinum working electrode in monomer free dichloromethane (with 0.1
M TBAPF6).The anodic wave at 0.8 V is due to release of
trapped charges (vide infra) from reduction. Cathodiccharge trapping,
present in complete overlap with the reduction at −0.6 V here,
is also observed clearly under monomer free conditions on an ITO working
electrode (Figure S22). (Right) Cyclic
voltammetry of a poly-APCNDI modified glassy carbon electrode
in monomer free dichloromethane. Initial scan toward negative potentials
from 0.0 V shows a reversible one electron redox wave (A) with a corresponding
discharge peak (B) on the return cycle toward positive potentials
which is absent on the second cycle in which the switching potential
is 0.3 V. The third consecutive cycle to positive and the negative
potentials shows a discharge peak due to trapped positive charges
(D) (with 0.1 M TBAPF6, platinumcounter, and SCE reference
electrode, scan rate 0.1 V s–1). SCE reference and
platinumcounter electrodes.
UV/vis–NIR Absorption Spectroelectrochemistry of poly-APCNDI
The UV/vis absorption spectrum of poly-APCNDI resembles
that of the monomer with the characteristic vibronic structure of
the naphthalene diimide unit red-shifted slightly (Figure S23). UV/vis absorption spectra of poly-APCNDI on an ITO on glass electrode in several oxidation states are shown
in Figure . Reduction
results in the appearance of a characteristic absorption band at 480
nm corresponding to the NDI monoanion (at −0.90 V), concomitant
with a decrease in the absorption of the NDI unit at 390 nm. At more
negative potentials, a band at 425 nm appears corresponding to the
NDI dianion (at −1.40 V), concomitant with a decrease in the
absorbance of the NDI monoanionat 480 nm (Figure ). Complete conversion to the NDI dianion,
i.e., a complete loss in absorbance of the NDI monoanionat 710 and
790 nm, was not achieved, indicating thatCoulombic interactions are
not fully compensated by uptake of cations (TBA+) from
the electrolyte. Scaled subtraction of the UV/vis absorption spectrum
of the NDI monoanion reveals the absorption spectrum of the NDI dianion
(Figure S24). Notably, subsequent oxidation
at 0.0 V does not lead to a full recovery of the original absorption
spectrum with residual absorbance of the NDI monoanionconsistent
with kineticcharge trapping in the film (Figure S25, vide infra). UV/vis spectra recorded during cyclic voltammetry
between 0.00 to 1.60 V showed the appearance of NIR absorptions assigned
to the monocationic (425 and 1200 nm, at 1.00 V, Figure S26) and dicationic (775 nm, at 1.5 V) states of the
bis-carbazole units (Figure ) and a decrease in bis-carbazole absorption at 325 nm. The
absorbance of the NDI unit is unaffected by oxidation. The combination
of NDI and APC units allow for access to five distinct
redox states and control of absorption over the entire UV/vis–NIR
spectral range, and in particular the visible region which is not
accessed easily with polymerscomprising of carbazole units alone.[70]
Figure 13
In situ UV/vis absorption spectroelectrochemistry of poly-APCNDI on an ITO slide (left) at 0.20 V (black), −0.90
V (light blue) and at −1.40 V (dark blue) and (right) at 0.00
V (black), 1.00 V (orange), 1.50 V (red), and at 0.00 V again (gray)
in dichloromethane (0.1 M TBAF6).
In situ UV/vis absorption spectroelectrochemistry of poly-APCNDI on an ITO slide (left) at 0.20 V (black), −0.90
V (light blue) and at −1.40 V (dark blue) and (right) at 0.00
V (black), 1.00 V (orange), 1.50 V (red), and at 0.00 V again (gray)
in dichloromethane (0.1 M TBAF6).
Resonance Raman Spectroelectrochemistry of poly-APCNDI
In
situ Raman spectroscopy, at λexc 785 nm allowed
for characterization of the APCNDI monocation, dication,
and monoanion states, making use of resonance enhancement due to the
absorption of these states at this wavelength (Figure , vide infra). Continuous monitoring by
Raman spectroscopy during cyclic voltammetry on a polymer modified
platinum electrode between 0.20 and 1.30 V shows the appearance of
weak bands at 1622, 1592, and 702 cm–1 upon oxidation
between 0.7 and 1.0 V. At potentials above 1.1 V, additional bands
were enhanced substantially also together with a change in the relative
intensity of the bands atca. 1600 cm–1. These bands
disappeared upon subsequent reduction. The increased intensity observed
for the dication state compared with that for the monocation state
is consistent with the increased absorbance at 785 nm for the former
(Figure ). The relative
intensity of the bands of the weakly scattering monocationic species
allows them to be distinguished easily from those of the dicationic
species and are in both cases assigned to the bis-carbazole unit.
Figure 14
(Upper)
In situ Raman spectroelectrochemistry of poly-APCNDI at
a Pt working electrode, scanning the potential from 0.7 to 1.3
V at 5 mV s–1 (in dichloromethane with 0.1 M TBAPF6, λexc 785 nm) and (lower) comparison of
the dication species formed at 1.3 V (i) and the monocation species
at 1.0 V (ii).
(Upper)
In situ Raman spectroelectrochemistry of poly-APCNDIat
a Pt working electrode, scanning the potential from 0.7 to 1.3
V at 5 mV s–1 (in dichloromethane with 0.1 M TBAPF6, λexc 785 nm) and (lower) comparison of
the dication species formed at 1.3 V (i) and the monocation species
at 1.0 V (ii).The resonance enhanced
Raman bands (at λexc 266
nm) of APCNDIat 1622 and 705 cm–1 (Figure ) are assigned
to C=C stretching and C–H out of plane bending of the
carbazole moieties and correspond with bands observed for the mono-
and dication states of poly-APCNDI. The bands at 1172
and 1020 cm–1 correspond to bands observed here
at 1164 and 1024 cm–1, assigned to in plane bending
of the oxidized carbazoleC–H modes. Additionally, the appearance
of a band at 1269 cm–1 was assigned as a C–N
stretching mode, which is close to the band observed at 1237 cm–1 in the spectrum of the monomer (at λexc 266 nm), the shift to higher wavenumber being consistent with the
increased bond strenght expected in the cationic state (i.e., increased
C=Ncharacter). The carbazoleC=C stretching band at
1622 cm–1 is unchanged upon oxidation, while the
stronger band shifts from 1594 to 1599 cm–1 (also
observed in the ex situ Raman measurements, vide infra) and gains
intensity relatively to the 1622 cm–1 band. Furthermore,
a shoulder at 1653 cm–1 is observed in the monocationic
state, assigned to the C=Calkene stretch due to loss of aromaticity
through the radical character of the monocation. The band at 704 cm–1 observed for the monomer at λexc 266 nm, assigned to a C–H out of plane bending mode of APCNDI, shifts to 712 cm–1 upon further
oxidation to the dicationic state. In the case of the dicationic state,
the bands at 1164, 1140, and 1092 cm–1 are assigned
as in plane, and 675, 651, and 618 cm–1 as out of
plane C–H bending modes, constituting shifts of up to 30 cm–1 from those modes observed in resonance Raman spectrum
of the monomer.
Charge Trapping in poly-APCNDI Films
In contrast to APCCDI, for APCNDI a prepeak
to both oxidation
and reduction waves was observed on a range of electrodes (including
glassy carbon, platinum, and gold macroelectrodes and ITO coated glass
slides), indicative of charge trapping.[71] For example, at a gold macroelectrode, additional redox waves were
observed at 0.80 V and at −0.50 V during formation of poly-APCNDI in the cyclic voltammetry of APCNDI (Figure ). Charge trapping
was first reported by Murray et al. in 1981[35] and is due to the confinement of charges in the polymer film through
defects (i.e., thermodynamic—where a distinct species with
a redox potential less positive or less negative than the polymer
is formed) or where the outer layer is unable to discharge before
the inner layer is depolarized (i.e., kinetic—where polymer
film is sufficiently thick that the inner layer insulates the outer
layer from the potential gradient at the electrode, Figure ).
Figure 15
poly-APCNDI film formation via repetitive cyclic voltammetry
at a gold macroelectrode (0.067 mM in dichloromethane with 0.1 M TBAPF6, scan rate 0.1 V s–1, inert atmosphere,
with Ag/AgCl reference and Pt counter electrode). Left: initial cycle(s)
and right: later cycles. The prepeaks “*” are due to
discharge of kinetically trapped charges.
poly-APCNDI film formation via repetitive cyclic voltammetry
at a gold macroelectrode (0.067 mM in dichloromethane with 0.1 M TBAPF6, scan rate 0.1 V s–1, inert atmosphere,
with Ag/AgCl reference and Ptcounter electrode). Left: initial cycle(s)
and right: later cycles. The prepeaks “*” are due to
discharge of kinetically trapped charges.The increase in the discharge peak current and shift to more
positive/negative
potential with cycle number and hence film thickness are apparent
during the polymerization of APCNDI by cyclic voltammetry
(Figure ). These
shifts reflect an increase in the distance between the outer edge
of the polymer film and the limit to the thickness of film at the
electrode thatcan be discharged directly. This, however, does not
imply thatcharge trapping does not occur in films of poly-APCCDI (vide supra), albeit that the trapped positive charges are not released
by film reduction due to the absence of an accessible reduction wave.
The formation and release of trapped charges can be observed by cyclic
voltammetry, UV/vis absorption (Figure ), and resonance Raman spectroscopy providing
dual redox-functionality of electrochromism and nonvolatile 3-state
memory (reduced, neutral, oxidized)Raman spectra recorded at
a poly-APCNDI modified Au
electrode enables identification of the species responsible for the
charge trapping, with spectra recorded, ex-situ, of charged films
showing Raman bands thatconfirm that the species responsible for
charge trapping are in both cases the one electron oxidized and reduced
states (Figure ).
Figure 16
Ex situ
Raman spectroscopy (λexc 785 nm) of a
poly-APCNDI modified Au working electrode. Recorded states
include the discharged (by cycling to −0.5 and 0.8 V in order
to release negatively (left) and positively (right) trapped charges,
respectively, solid black lines), charge trapped (by cycling to −0.9
V (left) or 1.1 V (right) and back, blue, and red lines), and fully
charged state (by pausing the cyclic voltammogram at either −0.9
(left) or 1.1 (right) V, cyan and orange lines). In dichloromethane
with 0.1 M TBAPF6 at a scan rate of 0.5 V s–1.
Ex situ
Raman spectroscopy (λexc 785 nm) of a
poly-APCNDI modified Au working electrode. Recorded states
include the discharged (by cycling to −0.5 and 0.8 V in order
to release negatively (left) and positively (right) trapped charges,
respectively, solid black lines), charge trapped (by cycling to −0.9
V (left) or 1.1 V (right) and back, blue, and red lines), and fully
charged state (by pausing the cyclic voltammogram at either −0.9
(left) or 1.1 (right) V, cyan and orange lines). In dichloromethane
with 0.1 M TBAPF6at a scan rate of 0.5 V s–1.C=C stretching modes at
1620 and 1594 cm–1 are observed, which correspond
to a one electron oxidized bis-carbazole
species. The spectrum of the positively charge trapped film shows
a shoulder at 1620 cm–1 and a shift toward 1594
cm–1 by the scattering maximumat 1598 cm–1. Additionally, Raman bands at 1341, 1267, 718, and 588 cm–1 appear both upon oxidation and in the film that had undergone a
cycle to positive potentials and subsequently to 0.0 V. Upon both
reduction of the polymer film and after a reductive cycle in which
the potential is returned to 0.0 V, bands at 1413 and 1374 cm–1 are observed. Furthermore, these bands decrease in
intensity concomitantly with the appearance bis-carbazole monocation
modes upon oxidation. The band at 1413 cm–1 is assigned
to a naphthalene aromaticC–C stretching by comparison with
the resonance Raman spectrum of APCNDI monomer recorded
at λexc 355 nm. Similarly, the bands at 541 and 1374
cm–1 correspond to those at 537 and 1386 cm–1, respectively, in APCNDI. Hence, positive
or negative charges trapped in the polymer film can be assigned as
due to kinetically trapped cationic and anionic forms of the bis-carbazole
and NDI moieties, respectively.Erasing and rewriting this three
state charge trapping system can
be achieved by application of positive and negative potentials (Figure ). Reduction of
the film followed by polarization of the electron to 0.0 V resulted
in the appearance of a discharge peak on cycling to positive potentials
even after a 30 min delay.
Figure 17
Sequential cyclic voltammetry of a gold macro
electrode poly-APCNDI modified film in monomer free solution
(dichloromethane
with 0.1 M TBAPF6, scan rate 0.1 V s–1, with Ag/AgCl reference and Pt counter electrode, “n-charging”
carried out by a reductive cycle to −0.9 V). Cyclic voltammograms
were recorded of a charged film, read-out after 30 min storage in
air while charged, a subsequently discharged film, and thereafter
immediately recharged film. Similar data showing charge storage over
6 days is shown in Figure S27.
Sequential cyclic voltammetry of a gold macro
electrode poly-APCNDI modified film in monomer free solution
(dichloromethane
with 0.1 M TBAPF6, scan rate 0.1 V s–1, with Ag/AgCl reference and Ptcounter electrode, “n-charging”
carried out by a reductive cycle to −0.9 V). Cyclic voltammograms
were recorded of a charged film, read-out after 30 min storage in
air while charged, a subsequently discharged film, and thereafter
immediately recharged film. Similar data showing charge storage over
6 days is shown in Figure S27.
Conclusions
The design of multifunctional
surfaces and especially redox functional
surfaces based on molecular components necessitates the proper orthogonal
functioning of not only the “active” components but
also the components required for polymer film formation. In this contribution,
we show that oxidative C–Ccoupling of carbazole is a versatile
approach to the formation of stable redox polymer films when two carbazole
units are tethered appropriately so as to enable sequential dimerization
and thereby stepwise polymer growth. The key advantage to the bis-carbazole
unit in polymer film formation is that the redox potential for the
oxidation of monomer is coincident with that of the second oxidation
of the bis-carbazole unit, thereby avoiding film growth limitations
seen with earlier systems. The unit connecting the two carbazole units
is key to achieving this and in the present study an amino phenyl
unit helps to lower the redox potential of the carbazole unit, however,
the use of a diimide group in the bridge is essential to preclude
interference by the formally, p-diaminobenzene motif.
The various precursors led to the design of the multifunctional electro-polymerizable
unit through insertion of an additional redox active naphthalene group
to form APCNDI. Interestingly, whereas poly-APCCDI shows redox switchable photoluminescence, the APCNDIDonor–Acceptor–Donor system exhibits complete quenching
of emission through intramolecular photoinduced electron transfer
between the NDI and APC moieties. The quenching
is sufficient to enable characterization of poly-APCNDI films in several redox states by resonance Raman spectroscopy. In
particular, we demonstrate thatcharge trapping in sufficiently thick
films of poly-APCNDI is kinetic and not thermodynamic.Although resonance Raman microspectroscopy is used in the present
study primarily to characterize the species responsible for charge
trapping as kinetic and not thermodynamic, read can be achieved by
UV/vis absorption spectroscopy and electrochemically. However, although
a possible advantage of Raman microspectroscopy is found in the specificity
of the molecular information contained within the spectra and high
spatial resolution, ultimately charge trapping is useful in electrical
readout systems despite the destructive nature of such readout. In
summary, the combination of facile polymer film formation with highly
controllable film thickness together with retention of the properties
of the monomer APCNDI in the films, provide for a 3-state
nonvolatile memory with nondestructive optical readout and by resonance
Raman spectroscopy.
Authors: Ryan E Dawson; Andreas Hennig; Dominik P Weimann; Daniel Emery; Velayutham Ravikumar; Javier Montenegro; Toshihide Takeuchi; Sandro Gabutti; Marcel Mayor; Jiri Mareda; Christoph A Schalley; Stefan Matile Journal: Nat Chem Date: 2010-05-16 Impact factor: 24.427
Authors: Jetsuda Areephong; Tibor Kudernac; Jaap J D de Jong; Gregory T Carroll; Davide Pantorott; Johan Hjelm; Wesley R Browne; Ben L Feringa Journal: J Am Chem Soc Date: 2008-09-04 Impact factor: 15.419
Authors: Philana Wesenhagen; Jetsuda Areephong; Tatiana Fernandez Landaluce; Nicolas Heureux; Nathalie Katsonis; Johan Hjelm; Petra Rudolf; Wesley R Browne; Ben L Feringa Journal: Langmuir Date: 2008-05-16 Impact factor: 3.882
Authors: Maaike T W Milder; Jennifer L Herek; Jetsuda Areephong; Ben L Feringa; Wesley R Browne Journal: J Phys Chem A Date: 2009-07-09 Impact factor: 2.781