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DOI: 10.1039/C8TC05774E (Paper) J. Mater. Chem. C, 2019, 7, 2987-2993

Organic electrochemical transistors from supramolecular complexes of conjugated polyelectrolyte PEDOTS†

Chiara Musumeci *a, Mikhail Vagin b, Erica Zeglio a, Liangqi Ouyang a, Roger Gabrielsson b and Olle Inganäs *a
aBiomolecular and Organic Electronics, Department of Physics Chemistry and Biology, Linköping University, SE-58183 Linköping, Sweden. E-mail: chiara.musumeci@liu.se; olle.inganas@liu.se
bLaboratory of Organic Electronics, Department of Science and Technology, Linköping University, SE-60174 Norrköping, Sweden

Received 16th November 2018 , Accepted 7th February 2019

First published on 13th February 2019

Abstract

Counterion exchange strategies are used to modify the hydrophilic character of the self-doped conjugated polyelectrolyte PEDOTS. The supramolecular complexes, soluble in organic solvents, are suitable to fabricate finely performing thin active layers in organic electrochemical transistors (OECTs). We demonstrate that ionic transport in these PEDOTS based complexes, thus their performance in OECT devices, is governed by a delicate balance among degree of doping, wettability and porosity, which can be controlled by a precise tuning of the polyelectrolyte/hydrophobic counterion ratio. We also show that the device operation can be modulated by varying the composition of the aqueous electrolyte in a range compatible with biological processes, making these materials suitable candidates to be interfaced with living cells.

Introduction

Conjugated polyelectrolytes are a class of (semi)-conducting polymers possessing charged groups covalently attached to the conjugated backbone. By enabling both electronic and ionic transport, they bridge the gap between electronics and biology, allowing the development of intimate bioelectronics interfaces.1 The charged side groups, making these materials soluble in polar solvents, allow for the incorporation of water molecules and mobile ions into the polymer matrix, leading to improved ionic conductivity with respect to conjugated polymers having hydrophobic side groups. Some conjugated polyelectrolytes are self-doped, meaning that the charged side groups act as counterions to balance the positive charges formed in the conjugated backbone upon oxidation.2 PEDOTS is a conjugated polyelectrolyte in which alkoxysulfonate side chains are covalently bound to a poly(3,4-ethylenedioxythiophene) (PEDOT) backbone. The negatively charged sulfonate groups render PEDOTS highly water soluble and stabilize the positive charges on the polymer backbone in its pristine oxidized conductive state, thus making PEDOTS a self-doped polymer with conductivity of tens of S cm−1.3 Changes in the level of oxidation also change PEDOTS conductivity, thus making it a suitable active material for the fabrication of functional devices, such as organic electrochemical transistors (OECTs).4–6 In a typical OECT, a gate voltage drives ions from an electrolyte into the bulk of the conjugated polymer, thus modulating its redox state and conductivity. Low voltage operation, high transconductance, and compatibility with operation in aqueous environment (e.g. biological media) make OECTs ideal devices to be coupled and interfaced with living systems and to work as active amplifying ion-to-electron transducers, ultimately increasing the signal-to-noise ratio with respect to traditional electrodes used for electrophysiology.7,8 The manipulation of the hydrophobic/hydrophilic character of these electrode materials may also have potential for the solid/liquid/gas interfaces found in fuel cells driven with gases.

The charged side chains of PEDOTS can also be exploited to fabricate new materials by supramolecular interactions. The negative sulfonate groups can in fact interact electrostatically with positively charged moieties, creating supramolecular complexes with new functionalities. This strategy has been specifically used for the fabrication of conductive fibers from biotemplates such as protein fibers9–12 and DNA,13 for the fabrication of multilayered electrochromic films14,15 and conductive hybrid nanocomposites.16 By using counterion exchange strategies, i.e. by replacing small counterions with ions bearing long hydrophobic chains, it is also possible to modify the hydrophilic character of PEDOTS, creating new materials which are soluble in organic solvents and can form films that are stable in aqueous electrolytes without the need of crosslinking.17 We have also shown that these materials can be used as active layers in OECTs,17 can be inserted into lipid membranes and used to modify biological functions in living cells.18 The OECTs based on these hydrophobic complexes, however, required relatively concentrated aqueous electrolytes (e.g. 1 M KCl) to be operational. We anticipate indeed that they show poor or null switching ability at electrolyte concentrations around 0.1 M (or lower), corresponding to physiological conditions where cells and biological systems function. Here we investigate the parameters affecting the operation of PEDOTS based hydrophobic complexes in OECTs, aiming to get guidelines for the design of these materials and their use in biologically compatible environment.

Results and discussion

PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA complexes having different compositions were obtained by mixing PEDOTS (from 1 mg mL−1 solutions) with dioctylammonium (DOA) at different molar ratios, namely 1[thin space (1/6-em)]:[thin space (1/6-em)]10, 1[thin space (1/6-em)]:[thin space (1/6-em)]1 and 2[thin space (1/6-em)]:[thin space (1/6-em)]1, with respect to the EDOTS monomer. Scheme and images relative to the different preparation steps are shown in Fig. 1. In the three cases the formation of the complex resulted in a blue precipitate, insoluble in water (Fig. 1d), which could be readily dissolved in chloroform/methanol 1[thin space (1/6-em)]:[thin space (1/6-em)]1 v/v (Fig. 1e). At first glance, the three solutions appeared slightly different in color. While the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 solution showed a light purple color, the other two appeared light blue. This color change, from purple to pale blue can be observed when PEDOTS is switched from the neutral to the oxidized state, as a consequence of the decrease of absorption of the π–π* transition at around 600 nm.3,12 Accordingly, UV-Vis absorption spectra of the three complexes (Fig. 1f) showed a higher level of dedoping for the 1[thin space (1/6-em)]:[thin space (1/6-em)]10 complex with respect to the other two complexes, demonstrated by the increased absorption at around 560 nm. The increased dedoping is likely due to a larger amount of DOA cations interacting with the sulfonate side groups of PEDOTS during the complex formation, and making them unavailable to stabilize the positive charges on the backbone. On the other side, the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1 showed the lowest absorption at 560 nm, indicating a higher level of oxidation of the PEDOTS backbone. PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 2[thin space (1/6-em)]:[thin space (1/6-em)]1 showed a similar spectrum to the 1[thin space (1/6-em)]:[thin space (1/6-em)]1 sample, indicating similar doping level.
image file: c8tc05774e-f1.tif
Fig. 1 Preparation of the PEDOTS:DOA complexes. (a) Scheme of the assembly of the complexes from the PEDOTS polyelectrolyte and dioctylammonium salt. (b) Solutions of PEDOTS after addition of the DOA at different PEDOTS/DOA ratios, namely 1[thin space (1/6-em)]:[thin space (1/6-em)]10, 1[thin space (1/6-em)]:[thin space (1/6-em)]1 and 2[thin space (1/6-em)]:[thin space (1/6-em)]1 with respect to the monomer. (c) Precipitation of PEDOTS:DOA hydrophobic complexes from aqueous solutions obtained after vortexing the solutions in (b). (d) Dry PEDOTS:DOA hydrophobic complexes. (e) PEDOTS:DOA solutions in chloroform/methanol. (f) UV-Vis absorbance spectra of PEDOTS:DOA complexes in chloroform/methanol.

Electrochemical transistors having PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 films as an active layer showed good switching properties when using electrolyte at high ionic strength, i.e. 1 M KCl, but scarce or null operation in 0.1 M KCl, as shown in Fig. 2a. Increasing the PEDOTS to DOA ratio to 1[thin space (1/6-em)]:[thin space (1/6-em)]1 led to improved operation in 0.1 M KCl, suggesting that a higher content of hydrophobic counterions in PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 may likely hinder both the ionic and electronic transport. However, the use of the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 2[thin space (1/6-em)]:[thin space (1/6-em)]1 did not seem to enable better device performance. On the contrary, these devices remained in the non-conductive state in the voltage range investigated (Fig. 2b).


image file: c8tc05774e-f2.tif
Fig. 2 Electrochemical transistors, OECTs. (a) Transfer characteristics (solid line, left axis) and transconductance (dashed line, right axis) of PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 in 0.1 M and 1 M KCl. (b) Transfer characteristics of PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10, 1[thin space (1/6-em)]:[thin space (1/6-em)]1 and 2[thin space (1/6-em)]:[thin space (1/6-em)]1 in 0.1 M KCl. The scheme of the devices is shown in the inset in (b). Additional curves for these devices are shown in Fig. S1 and S2, ESI.†

The ionic permeability of the different films at different ionic strengths was evaluated through cyclic voltammetry by using potassium ferricyanide as a redox probe (Fig. 3). The blocking properties of the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 at low ionic strength (0.1 M KCl) are demonstrated by the decreased current with respect to the one observed on bare gold microelectrodes. The increased currents in the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1 and 2[thin space (1/6-em)]:[thin space (1/6-em)]1 seem to indicate instead an improved ionic transport in these films. At higher ionic strengths, i.e. at electrolyte concentrations of 0.5 M and 1 M (Fig. 3b and c), current increases for all film compositions. However, the cyclic voltammograms of Fig. 3 also show increased capacitive background contribution at higher PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA ratios, as well as electrolyte concentrations, which makes an accurate evaluation of the redox current problematic.19 Peak currents, ip, increased linearly with the square root of the scan rate (ν1/2) as an indication of a diffusion-limited process (Fig. S4, ESI†). By fitting the ipvs. ν1/2 curves to the Randles–Sevcik equation we estimated the effective area in the different electrolyte concentrations (Fig. S1, ESI†) and observed that while the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 film showed only a 19% area increase with respect to the bare Au electrode in 0.1 M KCl, an increase of 72% was calculated for the 1[thin space (1/6-em)]:[thin space (1/6-em)]1 sample. Moreover, higher electrolyte concentration resulted in a larger increase for both samples, up to 81% with respect to the dilute solution for the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 and 113% for the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1 in 1 M KCl. These values suggest a different degree of swelling and ion uptake of the two samples.


image file: c8tc05774e-f3.tif
Fig. 3 Cyclic voltammetry of 2 mM K3[Fe(CN)6] in 0.1 M (a), 0.5 M (b) and 1 M (c) KCl for bare gold IDME and PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA films at different PEDOTS/DOA ratios.

To get more insight on the changes in electrolyte-accessible surface areas with varying the composition, we used a combined characterization through atomic force microscopy (AFM) and electrochemical impedance spectroscopy (EIS). AFM analysis showed a different morphology for the three films of comparable thickness (Fig. 4). Although AFM only images the top surface of the films, some information can be drawn when comparing the topography of the different samples. PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 shows a high surface roughness approximately two times larger than the other two films, and a decreasing surface area from the 1[thin space (1/6-em)]:[thin space (1/6-em)]10 to the 1[thin space (1/6-em)]:[thin space (1/6-em)]1 and the 2[thin space (1/6-em)]:[thin space (1/6-em)]1, as shown in Table 1. The low value of surface area difference, representing the ratio between the surface area and its projected area, in PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 2[thin space (1/6-em)]:[thin space (1/6-em)]1, indicate a higher level of compactness of the film, which may be the cause of the hindered ionic transport into the bulk of the film during OECTs operation. The highest roughness of PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 should instead favor ionic transport and enhance operation in these films, since the capacitance of an electrode is generally directly dependent on its surface area. However, capacitance can also depend on other parameters such as pore size distribution and surface chemistry. For activated carbon materials, for example, capacitance is higher for a sample with wider micropore size distribution than for a sample with higher surface area but too narrow micropore size distribution. In addition, a high amount of surface groups increase the capacitance of a porous electrode, either by improving the wettability of the material or by pseudocapacitance effects.20 The poor performance of PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 devices indicates that morphology and porosity of the electrode is not the limiting parameter in this case. Rather, its high hydrophobicity, being a consequence of a higher amount of DOA counterions in the complex, may likely be the cause of a lower degree of swelling and ion uptake in the aqueous electrolyte.4,21


image file: c8tc05774e-f4.tif
Fig. 4 AFM topography images of dry PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 (a), 1[thin space (1/6-em)]:[thin space (1/6-em)]1 (b) and 2[thin space (1/6-em)]:[thin space (1/6-em)]1 (c) films.
Table 1 Morphology parameters of the PEDOTS:DOA films measured by AFM analysis
PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]10 1[thin space (1/6-em)]:[thin space (1/6-em)]1 2[thin space (1/6-em)]:[thin space (1/6-em)]1
a The surface area difference represents the ratio between the surface area and the projected area (6400 μm2), relative to the images in Fig. 4a–c.
Thickness 325 nm 385 nm 340 nm
Roughness RRMS 219 nm 119 nm 96 nm
Surface area 6693 μm2 6572 μm2 6484 μm2
Surface area differencea 4.58% 2.68% 1.32%

To assess the interplay between wettability and porosity of the films with different PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA ratios, we performed impedance spectroscopy in different background electrolytes, i.e. 0.1 M KCl, 0.2 M KCl and 0.05 M KCl/0.05 M CaCl2 (hereby named KCl/CaCl2), having ionic strengths compatible with biological activity, such as that found in cell culture media.

Compared to the other two compositions, PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1 revealed a minimized total impedance (Fig. 5a) probably due to a balance between wettability and porosity and a decrease of total impedance with both ionic strength increase and calcium addition. The quantitative analysis of the impedance spectra of the gold electrodes modified with thin films of the complexes was done with the unified equivalent circuit shown in Fig. 5a. The presence of two time-resolved processes could be modelled by two RC elements in the unified equivalent circuit developed for an electrode covered with a porous coating.22,23 Due to the significant film conductivity at applied potentials higher than 0 V, the circuit has been reduced to a simple 4-element equivalent circuit. Since the boundary between the layers is not ideally smooth, a quantitative analysis of the electrode impedance response requires a more complicated, distributed circuit model featuring constant phase elements (CPE) rather than pure capacitors. The capacitance values have been calculated as:24

 
image file: c8tc05774e-t1.tif(1)
where Rs is the solution resistance, P is a fitting parameter of the CPE and ϕ is the fitted exponent factor, which varies from 0 to 1. When ϕ is equal to 0, the CPE behaves as a pure resistor and when ϕ = 1 the CPE represents a pure capacitor. The equivalent circuit providing the best fit consists of the solution resistance Rs and two parallel branches representing the diffusion through pores (pore resistance RP and pore capacitance (CPEP)) and the double layer capacitance (CPEDL). A single set of parameters has been used to simultaneously fit the real and imaginary parts of the impedance spectra over the frequency range from 0.1 Hz to 50 kHz (Table 2 and Table S1, ESI†). A value of the fitting quality parameter χ2 of ≤0.001 obtained for all spectra indicates a very good fit. Consistently with total impedance behavior, the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1 showed higher capacitance with respect to the other thin films, and up to 40 times decrease of pore resistance and slight increase of both capacitances with both ionic strength increase and calcium addition showing the ionic transport enhancement. PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1 revealed the lowest values of pore resistance and highest capacitance in 0.2 M KCl and KCl/CaCl2.


image file: c8tc05774e-f5.tif
Fig. 5 (a) Impedance spectra acquired on different film-modified gold electrodes in 0.1 M KCl. (b) Impedance spectra of PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1 in different background electrolytes. The solid lines represent the results of the fittings with the equivalent circuit shown in the inset in (a). Bias 0.2 V, 10 mV amplitude.
Table 2 Solution resistance (Rs), pore resistance (RP), pore capacitance (CP) and double layer capacitance (CDL) of the different films in the different background electrolytes, obtained from the fittings of the impedance spectra of Fig. 5, performed utilizing the unified equivalent circuit in Fig. 5a
PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA Electrolyte R s (W) C p (μF) R p (W) C DL (μF)
1[thin space (1/6-em)]:[thin space (1/6-em)]10 0.1 M KCl 135 0.14 3606 0.3
0.2 M KCl 76 0.3 606 1.9
0.05 M KCl, 0.05 M CaCl2 103 0.32 336 2.4
1[thin space (1/6-em)]:[thin space (1/6-em)]1 0.1 M KCl 121 0.24 7834 1.1
0.2 M KCl 81 0.89 165 5.5
0.05 M KCl, 0.05 M CaCl2 93 0.5 251 4.7
2[thin space (1/6-em)]:[thin space (1/6-em)]1 0.1 M KCl 119 0.2 8274 0.12
0.2 M KCl 59 0.3 1821 0.62
0.05 M KCl, 0.05 M CaCl2 87 0.22 518 0.23

We note that the concept of pore in these soft materials may be problematic. The swelling of the more-or-less hydrophobic complex in electrolytes is a dynamic process and includes formation of “pores” where solvent may insert, thus changing over time the distribution of pore size and tortuosity. We therefore treat these fitted parameters as very qualitative representation of the steady state geometry of the swollen polymer film.

To monitor the changes in conductance of the PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1 active layer as a function of the applied voltage in the different electrolytes we then used a four-electrode electrochemical setup comprising two working electrodes as source and drain contacts, a reference electrode and a counter electrode (see inset in Fig. 6a).17,25–28 In the three electrolyte solutions, the film showed a transition from a neutral, nonconducting form to an oxidized, highly conducting state, reaching channel resistances 2–3 orders of magnitude lower when changing the electrolyte from 0.1 M KCl to KCl/CaCl2 (Fig. 6a). As a result, the corresponding OECTs show greatly improved operation when KCl/CaCl2 was used as electrolyte (Fig. 6b). Also, while the current increases with the scan rate in 0.1 M KCl, the channel resistance was found to be completely independent on the scan rate in 0.2 M KCl or in KCl/CaCl2 electrolyte, suggesting that ions encounter very low resistance to penetrate the bulk film in these conditions.


image file: c8tc05774e-f6.tif
Fig. 6 Performance of PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA 1[thin space (1/6-em)]:[thin space (1/6-em)]1. (a) Channel resistance as a function of the gate voltage and at different scan rates in a four-electrode setup. The measurements were performed by varying the voltage at the CE (see scheme of the setup in panel (i)) while keeping 50 mV voltage difference between WE1 and WE2. The three panels refer to different electrolytes, as indicated in the legend. (b) Transfer characteristics of OECTs in different electrolytes.

Improved switching ability of an OECT at increased electrolyte ionic strength has been explained by both a faster ionic motion and the reduction of the Debye length with the concomitant increase in the density of ions that accumulate at the active layer.29

Another feature shown in Fig. 6 is a shift of the curves towards more negative voltages when going from 0.1 M KCl to 0.2 M KCl, and from 0.2 M KCl to KCl/CaCl2. Ion sensitive properties of OECTs have been observed in PEDOT:PSS based devices, with the transfer curves shifting to lower gate voltages at increased cations concentrations. The relative change of the gate voltage showed a logarithmic Nernstian dependence on the concentration of the electrolyte, with larger shifts in presence of multivalent cations, in accordance with the largest shift observed for our sample in the presence of bivalent calcium ions.30 We cannot exclude also a stabilizing role of the calcium ions when the devices are operated in KCl/CaCl2 (Fig. S3, ESI†). Crosslinking of PEDOTS with Ca2+ could indeed cause the polymer precipitation from solutions at pH above 8,13 and prevent detachment of thin films from solid substrates.31

Experimental

Poly(4-(2,3-dihydrothieno-[3,4-b]-[1,4]dioxin-2-yl-methoxy)-1-butanesulfonic acid, dowex-protonated) PEDOTS was synthesized as previously reported.3 Dioctylammonium (DOA) chloride 2.5 mM stock solution was prepared by dissolving dioctylamine (Sigma Aldrich) in 0.1 mM HCl and adjusting the pH to 4 (note that pH and concentration affect both DOA acid/base and solubility equilibria and have a big impact on the assembly of the complexes, see also ref. 18). MilliQ water having a resistivity of 18.2 MΩ cm was used for preparation of the aqueous solutions. Two-terminal gold interdigitated microelectrodes (IDME) on glass (MicruX Technologies) were used for electrochemical characterizations and device fabrication. All substrates were washed in an ultrasonic bath in water, acetone and isopropanol prior to film deposition.

PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA complexes having different compositions were obtained by mixing PEDOTS (from 1 mg mL−1 solutions) with DOA at different molar ratios with respect to the EDOTS repeat unit, namely 1[thin space (1/6-em)]:[thin space (1/6-em)]10, 1[thin space (1/6-em)]:[thin space (1/6-em)]1 and 2[thin space (1/6-em)]:[thin space (1/6-em)]1 (see Fig. 1b). Vortexing for 5 min resulted in the formation of precipitates of hydrophobic PEDOTS:DOA complexes (Fig. 1c), which could be isolated by successive cycles of centrifugation (10[thin space (1/6-em)]000 rpm, 10 min) and washing in 0.1 mM HCl to remove the excess of DOA or PEDOTS. Finally, the pellets were dried under nitrogen flux for 60 minutes (Fig. 1d). PEDOTS:DOA complexes were dissolved in methanol[thin space (1/6-em)]:[thin space (1/6-em)]chloroform 1[thin space (1/6-em)]:[thin space (1/6-em)]1, at a concentration of 1 mg mL−1 with respect to PEDOTS. For UV-Vis absorbance spectra, all solutions were diluted to 0.05 mg mL−1.

Cyclic voltammetry of the PEDOTS:DOA films deposited on IDME was performed on a Autolab/PGStat10 (Ecochemie, The Netherlands), by using Ag/AgCl and a platinum wire as reference and counter electrodes, respectively. 2 mM K3Fe(CN)6 was used as redox probe, with KCl at different concentrations as supporting electrolyte.

For the 4-electrode electrochemical measurements, PEDOTS:DOA complexes were drop cast on the IDME on glass. Measurements were performed on an Autolab type III bipotentiostat (Metrohm Autolab, The Netherlands). In this setup, the two gold terminals constituted two working electrodes (WE1 and WE2), while Ag/AgCl (3 M KCl) and a platinum wire were used as reference and counter electrodes, respectively. Measurements were carried out by measuring the current at the working electrodes while changing the voltage at the CE (which corresponds to a gate electrode in the OECT configuration), while keeping the voltage difference between WE1 and WE2 constant. Resistance values were obtained by subtracting the current response at a voltage difference ΔVWE = 50 mV with the one at ΔVWE = 0 mV.

Electrochemical Impedance Spectroscopy (EIS) of the PEDOTS:DOA films deposited on IDME was performed on an Autolab type III bipotentiostat (Metrohm Autolab, The Netherlands).

Electrochemical transistors (OECTs) were fabricated by drop casting few microliters of the PEDOTS:DOA complexes in chloroform/methanol on the IDME and using Ag/AgCl as gate electrode. Potassium chloride (KCl) and calcium chloride (CaCl2) at different concentrations and ratios were used as electrolytes. A scheme of the devices is shown in Fig. 2b. The electrical characterization of the devices was performed on a Keithley 4200 parameter analyzer, in air and at room temperature. The measurements were performed at a scan rate of 20 mV s−1. All the transistors had the same channel length (L = 20 μm) and width (W = 39[thin space (1/6-em)]000 μm).

Atomic force microscopy (AFM) of the dried films was performed in tapping mode with a Dimension 3100/Nanoscope IIIa system, by using commercial silicon cantilevers with a nominal spring constant of 40 N m−1. Films thicknesses measured by AFM on representative devices were 325 nm for the 1[thin space (1/6-em)]:[thin space (1/6-em)]10, 385 nm for the 1[thin space (1/6-em)]:[thin space (1/6-em)]1 and 340 nm for the 2[thin space (1/6-em)]:[thin space (1/6-em)]1 PEDOTS[thin space (1/6-em)]:[thin space (1/6-em)]DOA films.

Conclusions

We have shown that ionic transport in PEDOTS based complexes is governed by a delicate balance among degree of doping, wettability and porosity, and that these parameters can be controlled by engineering the supramolecular assembly through a precise tuning of the polyelectrolyte/hydrophobic counterion ratio. We have also shown that is possible to improve OECT operation by slightly increasing the ionic strength of the electrolyte or by adding bivalent calcium ions, while maintaining it in a range compatible with biological operation. This material is therefore suitable to operate at cell interfaces.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

This work was supported by the Knut and Alice Wallenberg foundation, through a Wallenberg Scholar grant to O. I., and Advanced Functional Materials (AFM) at Linköping University – a Swedish Government Strategic Research Area.

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Footnote

† Electronic supplementary information (ESI) available. See DOI: 10.1039/c8tc05774e
This journal is © The Royal Society of Chemistry 2019