Combining Electrospinning and Electrode Printing for the Fabrication of Stretchable Organic Electrochemical Transistors

Stretchable conductors and organic electrochemical transistors (OECT) were fabricated from PEDOT:Tos (poly (3,4-ethylenedioxythiophene):iron tosylate) nanofibers. The devices were prepared by a combination of electrospinning and electrode printing followed by vapor phase polymerization (VPP). The impact of both the processing time and the composition of three electrospinning mixtures on the electrospun fiber mats was evaluated by scanning electron microscopy and cyclic voltammetry. Fibrillar mats prepared from the different mixtures maintained their electrical properties and could be stretched up to 140% of their original length. Stretchable OECTs were fabricated by printing silver drain and source electrodes directly on the conductive spun fibers. The fabricated devices showed transistor behavior up to ∼50% strain.


INTRODUCTION
Interest in plastic electronics has been fuelled by the development of new synthetic methods for preparing conjugated organic materials, that enable organic electronics such as OLEDs, OPVDs, and OFETs [1][2][3]. Research in this field has further been motivated to bring the intrinsic properties of plastic electronics to fruition. Towards this end, efforts have focused on exploiting the environmental advantages of devices. For example, the efficiency of clean electricity production from sustainable resources using OPVDs continues to improve [4]. Similarly, advances in OLEDs materials result in reduced power consumption and increased efficacy [5].
The virtues of plastic electronics also include their processability. They can be cast from inks using various deposition methods such as spray and sheet coating along with roll-to-roll printing [6,7]. The advantages of these processing methods is their upscaling with the potential of production-scale device fabrication. These methods of printing conjugated materials that enable plastic electronics can further be applied to a range of substrates that have various mechanical properties. The inks can be applied to rigid and flexible substrates alike, opening the possibility of fabricating conformal devices whereby they can adopt a gamut of shapes and sizes including curved surfaces. This is in contrast with contemporary devices that are fabricated on rigid substrates. Stretchable electronic devices including light-emitting diodes [8], transistors [9] and solar cells [10] have been successfully developed. The virtues of merging flexibility and stretchability into devices give them mechanical properties that are ideally suited for their use in wearable electronics. Indeed, wearable plastic devices have found uses in a range of consumer electronics and healthcare applications.
Stretchable and flexible substrates cannot exclusively render devices wearable. Rather, each component that is integrated into devices must be complementary in their stretchable and bendable behavior. This ensures the layers respond to body motions in concert, resulting in a positive experience by the user when wearing the device. Although the stretchability and flexibility of the device components are critical mechanical properties of wearable electronics, their electrical response must be consistent with applied stress and strain. Given intrinsically conductive electrodes underpin the electrochemical performance of devices, the conductivity of these conjugated organic materials must not be compromised under the typically mechanical stresses and strains that are encountered when wear electronics. Indeed, this remains the principal challenge of the field, despite the many fabrication [11] and performances [12,13] improvements of stretchable devices.
Poly 3,4 ethylenedioxythiophene (PEDOT), doped with various counterions is ubiquitously used in plastic electronics owing to its high intrinsic conductivity and its processability. Despite these key properties, its rigid conjugated framework limits its capacity to deform. It further suffers from a dramatic loss of electronic conductivity with applied strain and stress. The limited mechanical properties of PEDOT based materials therefore makes it incompatible for use in truly flexible and stretchable devices. Its elongation at break can, however, be improved by blending it with a plasticizer. The plasticizer inserts between the macromolecular chains and it absorbs the external strain [14,15]. Different fabrication processes have been developed to make the mechanical properties of PEDOT compatible for its use in wearable electronics, while preserving its intrinsic conductivity. Strategies towards this end include depositing on a pre-strained elastomeric substrate [16], the Kirigami method [17,18], and electrospinning [19][20][21]. In the latter, non-woven fibers are formed by applying a high voltage bias between a given collecting surface and a polymer solution. The continuous collection of the fibers on the substrate forms a mat consisting of highly entangled fibers. The degree of entanglement and hence the thickness of the mat on the surface depends on the deposition time. The virtue of electrospun coatings is the stretchability of otherwise rigid polymers that is governed by the polymer chain entanglement.
The collective flexibility and stretchability of the electrospun coatings along with the straightforward fabrication make electrospinning an ideal process for preparing stretchable conjugated polymers. Indeed, a range of conjugated polymers have been electrospun including polyaniline [22], P3HT [23], polypyrrole [24,25] and PEDOT [26][27][28]. Extensive investigation have correlated the impact of the electrospinning solution viscosity on both the conductivity of the electronpun fiber and the fiber's morphology [29]. It is further known that the diameter of the electrospun fiber can be modulated by modifying the viscosity of the electrospinning solution [29]. Similarly, the morphology of the fibers can be varied with the use of cosolvents and their orientation can be adjusted by the combination of using different electrodes and varying the applied voltages [30]. Since the morphology of the fibrillar conductive mat significantly impacts its electronic properties, their conductivity can be optimized by adjusting the electrospinning solution.
Despite being a viable method for preparing conductive materials electrospinning is incompatible for directly preparing fibers of PEDOT. This is a result of these conjugated polymers being insoluble in the solvents that are compatible with electrospinning [31]. The spinnability of conjugated polymers can be improved by using carrier polymers such as poly (vinylpyrrolidone) (PVP) [32], poly (vinyl alcohol) (PVA) [33] and poly (ethylene oxide) (PEO) [34]. However, blending these insulating polymers in the electrospinning mixture generally reduces the overall conductivity of the resulting non-woven mat. While electrospun conductive fibers are possible with carrier polymers [19,20], the correlation between the composition of the electrospinning solution and the resulting conductivity of the electrospun fiber mats remains relatively undefined.
In light of the critical role that PEDOT plays in enabling electronic devices, there is a need to understand the influence of the electrospinning solution composition on the fibers' conductivity. More importantly, the interplay of the electrospinning mixture composition on the conductivity behavior of PEDOT fibers as a function of fiber stretching and bending needs to be established. This knowledge is of importance for spinning conductive fibers that meet the electronic and mechanical performance requirements for their use in wearable electronic devices. We were therefore motivated to prepare conductive PEDOT:Tos fiber mats by first electrospinning fibers followed by vapor phase polymerization. Three electrospinning mixtures, composed of carrying polymers (PEO and PVP) and varying amounts of oxidant (iron tosylate), along with different spinning times were investigated to understand the effect of electrospinning composition on electronic properties and the stretching behavior of the resulting conductive fibers. To validate the method developed for preparing fibers having suitable conductive and mechanical properties for their use in wearable electronics, the conductive mat was used in a stretchable organic electrochemical transistor (OECT). The conductivity and morphological dependency of PEDOT fibers on the electrospinning mixture composition, their stress/strain dependent conductivity and their use in a proof-of-concept stretchable transistor are herein described.

Preparation of Electrospinning Solutions
Three different electrospinning mixtures (A, B and C) were prepared as per below. Before adding CB54 v3, all mixtures were stirred with a magnetic stirrer until the polymer was completed dissolved.
The solutions were stirred with a magnetic stirrer during 10 h at room temperature to ensure the complete dissolution of the polymer carriers (PEO and PVP).

Electrospinning
The electrospinning setup includes a RT-collector (Linari Engineering) equipped with a cylindrical collector connected to a high voltage power supply. The electrospinning solution was injected through a 10 ml syringe equipped with a 0.8 mm diameter needle (Linari Engineering) and the injection flux was ensured by a computer-driven pump (Spraybase) at 0.1 ml/h. The relative humidity in the electrospinning hood was maintained between 18 and 23%. All fibers were electrospun at a 10 kV voltage with a distance of 22 cm between the needle and the collector. The collector translation speed was fixed to 20 mm/s and at 500 rpm. The spinning parameters were chosen such that fibers would exclusively be produced without any visible spray and droplets.
The process resulted in a non-woven mat of microfibers composed of the carrying polymer, imidazole, and iron tosylate. Three electrospinning times (700, 1,000 and 1,500 s) were chosen to study the effect of the fiber density on the electronic properties. The fibers were spun on different substrates depending on the required measurement: poly (ethyleneterephtalate) (PET) sheets for sheet resistance and transistors measurements, carbon paper for the electrochemical characterization and poly (dimethylsiloxane) (PDMS) for the stretching tests.

Spin Coating
Spin coating was performed with an Ossila Spincoater. The polymer mixtures used for electrospinning were diluted by a factor of two to allow spincoating of thin films (200-300 nm). Homogenous films for conductivity measurements were obtained on 25 mm 2 glass slides. For the stretching tests, the films were deposited on PDMS substrates.

Vapor Phase Polymerization
The fibers and spin coated films were subsequently transferred to a vapor phase polymerization (VPP) chamber for polymerization.
VPP of EDOT was carried out in a vacuum oven at 45 mBar and 50°C for 24 h. A Petri dish containing EDOT (1 ml) was placed in the lower part of the oven and the samples to polymerize were placed on top. A color change from yellow to light blue confirmed the formation of PEDOT around the fibers and on the spincoated films (Supplementary Figure S1). After VPP, the carrying polymer, unreacted species, and the undesired side products were removed by soaking the polymerized fibers (or films) in a deionized water (DI) bath for 10 min followed by a short rinsing step with EtOH and then water. These are referred to herein as the electrospun fibers (or spincoated films).

Characterization of Fibers and Films
Optical images of the fibers were obtained with a Zeiss Imager M1 microscope equipped with an AxioCam MRm camera (Carl Zeiss). Scanning electron microscopy images were obtained after metallization of the samples with gold for 50 s, using a scanning electron microscope fitted with a field emission gun (JEOL JSM7600F). Distributions of the fiber's diameters were calculated using the software ImageJ, based on SEM pictures. The thickness of the spincoated films was measured with a stylus profilometer (DektakXT Brucker). The sheet resistance was measured with a 4-point probe system (Ossila). The average value of the sheet resistance for each mixture was calculated from five arbitrary chosen regions per sample from five individual samples. Electrochemical measurements were carried out with a potentiostat (Biologic SP 300) and the data were recorded with Ec-lab software. Cyclic voltammetry was performed after bubbling N 2 in the electrolyte solution. Potentials were measured relative to an Ag wire that was used as a pseudoreference electrode in a three-electrode setup with a platinum mesh counter electrode. The working electrodes were electrospun fibers deposited on a 25 mm 2 carbon paper. Electrical measurements were performed under ambient conditions with an electrical probe station equipped with a Keysight B2900A source measure unit controlled with a Labview software. The stretchability tests were done with a LabVIEW softwarecontrolled tensile tester.

Transistor Fabrication
Organic Electrochemical Transistors (OECTs) were prepared from either electrospun fibers on PET substrates or spincoated films on glass substrates. The fabrication process is schematically represented in Figure 1. Fibers or films were covered with a PET stencil mask for plasma etching to form 12 PEDOT patterns. The PET stencil masks were fabricated using a ScanNcut SDX 1200 Brother cutting machine. The patterns were 2 mm wide and 15 mm long. The samples were etched for 1 h at 100 W and 50 sccm of O 2 (Plasmionique FLR 300H). Silver electrodes 11 mm long and 2 mm wide were printed with a Voltera Circuit Printer. The activated carbon gate electrode for aqueous gating medium was prepared using a carbon ink containing activated carbon (28 mg ml −1 ) and Nafion (1.4 mg ml −1 ) in isopropyl alcohol. The carbon ink was drop-casted on the carbon paper (Spectracarb 2050) and subsequently heated at 60°C for 5 h to remove solvent traces. The electrode was then confined in a glass cylinder (Φ 7 mm) that was filled with a NaCl solution (0.1 M) as the electrolyte and connected to the gate of the instrument.
Stretchable OECTs were prepared as previously reported, using a PDMS substrate [16]. Glass cloning cylinders were replaced by PDMS wells so the gate electrode could sustain the applied strain without breaking. Similarly, the printed silver drain and source electrodes were replaced by EGaIn to further allow the device to be stretched without breaking the contacts.

Morphology of Electrospun Fibers
Fibers were prepared by electrospinning either the PEO or the PVP solutions, as per Table 1. These polymers were chosen because they are ideal carriers for combined electrospinning and vapor phase polymerization of PEDOT [35,36]. The concentration of the polymers was kept below 1 wt% because a low concentration permits to obtain fibers with a smaller diameter. These were expected to show consistent conductivity with an applied strain. In contrast, fibers with larger diameters were expected to suffer from an undesired decrease in conductivity with applied stress/strain. Clevios CB54-V3 was used as the main component in the mixture to enrich the carrier polymer in the oxidant, thus providing a sufficient number of polymerization sites during VPP. Imidazole was added in a ratio of 0.5% mole relative to the iron tosylate to prevent acidic side-reactions that can arise from the two protons that are formed per degree of polymerization [37]. Two molecular weights of PEO were chosen in part because of their commercial availability. The two chosen molecular weights of PEO are known to form continuous fibers, while being consistent with the molecular weight of the extremely hygroscopic PVP that was also used in the study. The benefit of PEO is that it can be dissolved in minimal amounts of solvent, unlike PVP, resulting in spinning solutions with low viscosities. With the higher molecular weight of PEO, its amount in the electrospinning mixture could be reduced to 0.3 w% without compromising its spinnability. The diameter of the electrospun fibers can be adjusted with the solvent viscosity by varying either the amount of the solvent or the polymer content.
The SEM images revealed a difference in the fiber morphology contingent on the electrospinning composition. Qualitative differences in the fibers obtained from the two PEO mixtures are evident in Figures 2A,C). The Mixture B produced homogeneous fibers, whereas those produced from Mixture A are heterogenous. Indeed, both fine needle and bulb-like regions are formed on the same fibers along with the fibers having different thicknesses. Such is the case where multiple fibers of different diameter intersect. The resulting multiple bulb-like crossing points skew the mean average calculated diameter. This aside, randomly orientated fibers that are well-formed on the PET substrate ( Figure 2) were observed regardless of the electrospinning mixture. The different molecular weight of the carrying polymer in mixtures A and C led fibers with distinct diameters. The diameter of the as-produced fibers was the largest with the higher molecular weight of PEO in Mixture C. This is a result of its increased intrinsic viscosity relative to Mixture A, according to the Mark-Houwink relationship [38]. The diameter distribution of the fibers produced from Mixture A was bimodal, centered around 300 with a shoulder at 650 nm. In contrast, the diameter distribution from Mixture C had a typical Gaussian distribution with a maximum diameter around 2000 nm ( Figure 3). The fibers from mixture B were consistent with those from Mixture A, but with a broader distribution. There was also a difference in the ratio of the two dominant diameter distributions: 2:1 for A and 1: 1 for B for the diameters centered at 264 and 616 nm on the one hand and 396 and 748 nm on the other hand.

Electrical Properties
Considering a conjugated polymer to be a blend of metallic-like grains embedded in a non-conductive and disordered environment, its conductivity is expected to be governed by inter-grain electron transfer. The dense packing, high degree of polymer ordering, and limited defaults of small fibers can collectively promote electron transfer between the metallic-like domains to make small fibers more conductive than large fibers [39]. The electrical properties of the fibers were evaluated in terms of their sheet resistance rather than conductivity. This was because the sample thickness could not be defined. The effect of electrospinning time along with the composition of the spinning mixtures on the fibers' sheet resistance were evaluated. The sheet resistance was found to decrease with increasing electrospinning time ( Table 2). This was expected, due to the higher substrate coverage and the higher number of fiber junctions formed with longer spinning times. There is nearly a twofold decrease in the sheet resistance upon increasing the spinning time from 700 s to 1,000 s, while no improvements were in observed when increasing the spinning time to 1,500 s. This implies the minimum number of junctions that is required to reach the intrinsic conductivity limit of the fibers is formed at 1,000 s. These values are consistent with those reported in the literature for different PEDOT electrospun fibers [28,[40][41][42]. There was no significant difference in the sheet resistance between the longitudinal and transversal electrospinning direction. Assuming the electronic percolation between the chains at their crossing junction is the transport limiting process in the fibers, the consistent conductivity implies a large number of fiber junctions.
While the sheet resistance of fibers obtained from the mixtures A and C were similar, that of fibers obtained from mixture B was remarkably larger. This can in part be attributed to the morphological differences of the fibers. The fibers spun from PEO had fused junctions and they adopted a 2D arrangement, in contrast to the PVP spun fibers that were superimposed. The PVP fibers were stacked and a 3D arrangement was maintained where the fibers intersected. This topology was further expected to enhance the mechanical properties (vide infra).
Conductivity measurements were carried out on samples spincoated from the same mixtures having a similar thickness (ca. 200 nm). As per Table 3, the homogeneously smooth spincoated films have consistent conductivities ranging from ∼200 to ∼250 S cm −1 . The measured sheet resistances were similar to those of the fibers electrospun for 1,000 and 15,000 s in the case of the Mixtures A and C. The fibers

Electrochemistry
The electrospun fibers were further assessed by cyclic voltammetry. This was to evaluate the effect of the spinning time and the polymer carrier on the electrochemical properties of the fibers. More specifically, the quantity of charge transferred with an applied potential, and hence the doping/dedoping capacity of the fiber, can be assessed from the area of a potential vs. current voltammogram. Large areas of the voltammogram are indicative of greater doping/dedoping. Since the spinning time affects the number of fibers that are deposited on the surface along with the number of fiber junctions, the area of the voltammograms depends on the spinning time. The integrated area of the voltammogram for the fibers prepared from the mixture A was indeed greater than the other two mixtures (Figure 4). The relative order of the integrated areas was further consistent with the measured sheet resistance. This confirms the presence of fused fibers and a higher surface area induced by a smaller diameter distribution enhanced conductivity of the electrospun mat. The absence of a well-defined redox process in the cyclic voltammograms confirms the nonexistence of a discrete electron transfer process. It further implies that charge transfer processes take place over a broad range of potentials. This is consistent with a double-layer capacitance in an electrical double layer, common to the three spinning mixtures [43,44]. Meanwhile, the symmetry of the voltammograms confirms that the fibers can be reversibly doped and undoped with an applied potential with minimal loss of charge. This is a required behavior for use in OECT [45]. The conjugated organic components of OECTs make them suitable for use in both in vivo and in vitro bioelectronics. Similar to other plastic electronics, the mechanical properties of OECTs can be tailored by the judicious choice of the substrate that is used for their fabrication.
A key electrochemical parameter for assessing the suitability of the fibers for used in OECT is their specific capacitance. This can be calculated by integrating the voltammogram, providing the weight of active material is accurately known. Unfortunately, variabilities in the fabrication preclude accurately quantifying the amount of the deposited spun fibers. Given the conductive mats were prepared using similar parameters, the quantity of the fibers deposited for each mixture for the specific electrospinning time is understood to be consistent. The specific capacitance of the fibers prepared from the mixtures A, B, and C were estimated to be about 39, 13 and 25 F/g, respectively (see Supplementary Material). This is possible by comparing the integrated area of the voltammograms of the fibers for the same scan speed. However, the amount of PEDOT:Tos fibers deposited on the carbon paper can be estimated from the electrospinning flow rate, the density of the PEDOT and the surface of the carbon paper used for  a Errors are given from the range and the correction factor used for each measurement and these were averaged for the five sampled areas. Frontiers in Physics | www.frontiersin.org August 2021 | Volume 9 | Article 708914 6 electrochemical measurements. The specific capacitance of the fibers from the mixture A is greater than the other mixtures. This behavior can be ascribed to two factors. On one hand, there are more fiber junctions for the mixture A compared to the other samples. This results in the fiber's better overall conductivity and its smaller sheet resistance. On the other hand, the fibers from the mixture A had the smallest diameter relative to the other samples. This affords them a higher specific area and hence a greater electroactive surface area, collectively contributing to its greater capacitance.

Electromechanical Testing
Our electrospun fibers were evaluated to see whether they had a consistent conductivity with applied strain. This would make them suitable for stretchable transistors. The stretching of the fibers was assessed by monitoring their current during consecutive stretching cycles. The current as a function of applied strain for the three mixtures and for the three electrospinning times were measured. The fibers obtained from 1,500 s of electrospinning showed the highest current among the three spinning times, consistent with the sheet resistance measurements. All the three samples could undergo at least 80% of strain without significant changes in their sheet resistance. Remarkably, the fibers prepared from Mixture B could be stretched upwards of 140% strain, courtesy of its nodeless morphology. This allows most of the fibers to freely glide upon applied strain without breaking. At this stretching level, the sheet resistance decreased by only ∼15% (Figure 5B). The limited current loss of this sample with strain nonetheless makes it a promising candidate for use in stretchable electronic devices. A similar mixture was previous reported to yield fibers that could be stretched beyond the stretching limit of PDMS (160%), while retaining 15-20% of the initial current [35]. Stretching/releasing cycling tests also showed 50% of the initial current was retained and the current was consistent after only 30 cycles. Also, Shaker et al. reported a high current retention at 40% strain of PEDOT:PSS fibers that were prepared by wet electrospinning on a polyurethane matrix [46].
The capacity of the fibers to rearrange and dissipate the strain when stretched were qualitatively evaluated from the pictures that were taken with different applied strains (Supplementary Figure  S2A-C). The images show the fibers are progressively damaged (Supplementary Figure S2D-G) when stretched. The onset of the fiber damage for Mixture B occurred at ∼40% strain at which point the fibers lost their linear shape and they curled. No cracks were observed within the fibers from the mixture B, even with ∼120% strain. This is in contrast with the samples that spincoated on PDMS, which cracked at lower applied strains (white clusters Supplementary Figure S2F).
To validate the enhanced stretching capacity of the electrospun samples, their performance was compared to the three mixtures that were spincoated on PDMS. For this, the PDMS was pre-strained to 30% and the samples were then subsequently spincoated [16]. These films adopted a wavy shape when the substrate returned to its normal shape after the applied strain. The spincoated films on PDMS that were not pre-strained broke below 10% strain (Supplementary Figure S3), mainly due to the rigid structure of the PEDOT chains that prevents them from reorganizing and absorbing the strain when stretched. In contrast, the samples that were prepared on pre-strained PDMS could sustain the five stretching cycles at 20% strain but broke at 30% strain, owing to their buckling.
This aside, the PEDOT fibers produced from the three Mixtures could be stretched up to a minimum of 60% strain. The consistent current between the electrospun (1,500 s of electrospinning) and spincoated samples ( Figure 5D) confirms that the fiber shape, which is underpinned by the electrospinning process, does not affect the intrinsic electronic properties of PEDOT. The fibers can sustain mechanical deformation under strain because they can reorganize their structure with strain, unlike spincoated films. More importantly, both the mechanical and electronic properties of the final material can be tuned by adjusting the number of fused junctions in a fiber mat.

Organic Electrochemical Transistors (OECTs)
OECTs were fabricated from both electrospun ( Figure 6) and spincoated (Figure 7) samples. The output and transfer characteristics of the as-prepared OECTs showed the typical p-type behavior of PEDOT OECTs operating in depletion mode. Electrospun OECTs prepared from the mixture A showed the best performances. Transistors prepared from spincoated PEDOT showed similar performances to the electrospun fibers, but with higher ON/OFF ratios (∼45). This is consistent with a uniform and similar film morphology that is adopted over the entire surface of the device. In contrast, the fibers adopted unique morphologies Frontiers in Physics | www.frontiersin.org August 2021 | Volume 9 | Article 708914 8 that were highly dependent on the composition of the spinning solution and the spinning time. The larger ON/OFF ratios that were observed for the thin spincoated films can be ascribed to the larger contact area of the polymer with the gating medium between the source and the drain terminals compared to the fibers. However, as shown below, the spin coated devices have limited strain performance with respect to fibers.
Fibers produced from the mixture B showed the best results during the stretching tests while the ones produced from A led to higher currents, making both of them promising for use in stretchable transistors. Transistors were successively strained in 10% increments and both their transfer characteristics were subsequently recorded (Figure 8).
The transistors prepared from the mixture A ceased to work beyond 30% strain, while those from Mixture B functioned up to 50% strain. The OECTs fabricated from Mixture A had ON/OFF ratios that were about 10-fold greater than the devices prepared from Mixture B. Overall, the performance of the transistors prepared from Mixture B was less sensitive to the strain. This is a result of the greater degree of freedom of the fibers and the reduced number of fiber junctions for B relative to A. These distinct features stem from the different fiber morphology that is adopted by the two carrier polymers and from the different density and the number of fused junctions. Indeed, the conductivity of the resulting mat correlates with the number of fused fibers, which in turn, affords more electronic pathways. The tradeoff to this morphology is a reduced elongation at break because the fibers cannot contiguously slide and rearrange without breaking an electronic junction.

CONCLUSIONS AND PERSPECTIVES
Three electrospinning mixtures were prepared to investigate the impact of their composition on the morphology and the electrical properties of the resulting conductive PEDOT:Tos fibers. Conductive fibers were successfully prepared by the vapor phase polymerization of EDOT on the electrospun carrier fibers. The composition of the electrospinning solution and the spinning time led to distinct differences in both the distribution of the diameter and the number of junctions of the conductive fibers. Fibers with a smaller diameter distribution and a greater number of fiber junctions were the most conductive. These fibers also had the greatest specific capacitance owing to their larger specific electroactive area. The electrospun conductive fibers had enhanced stretchable and conductive  properties compared to spin coated thin films of PEDOT:Tos. Indeed, the conductivity of the fibers decreased by only 16% when stretched to 140% in length. This is due to their capacity to reorganize their structure with strain. The fibers could also be used in stretchable OECTs. Devices prepared from the fibers acted as OECTs under successive strains from 0 to 50%. Our results illustrate that conductive wires for use in stretchable electronics can be prepared from straightforward methods. By controlling the fiber morphology and their junction density, possible by readily tuning parameters such as polymer carrier and spinning time, stretchable electrodes having consistent conductivities when stretched can potentially be fabricated.

DATA AVAILABILITY STATEMENT
The raw data supporting the conclusions of this article will be made available by the authors, without undue reservation.

ACKNOWLEDGMENTS
The Natural Science and Engineering Council Canada (NSERC) is acknowledged for Discovery Grants awarded to FC and WS that enabled this collaborative research. This research is supported by Defence Research and Development Canada through an IDEaS Micronet (CFPMN1-008) grant awarded to FC. Equipment and infrastructure used for this research were acquired and maintained by the Canada Foundation for Innovation and Quebec Strategic Networks (CQMF-QCAM, RQMP, and GCM).