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Alcohol-based highly conductive polymer for conformal nanocoatings on hydrophobic surfaces toward a highly sensitive and stable pressure sensor


Conformal and ultrathin coating of highly conductive PEDOT:PSS on hydrophobic uneven surfaces is essential for resistive-based pressure sensor applications. For this purpose, a water-based poly(3,4-ethylenedioxythiophene) polystyrene sulfonate (PEDOT:PSS) solution was successfully exchanged to an organic solvent-based PEDOT:PSS solution without any aggregation or reduction in conductivity using the ultrafiltration method. Among various solvents, the ethanol (EtOH) solvent-exchanged PEDOT:PSS solution exhibited a contact angle of 34.67°, which is much lower than the value of 96.94° for the water-based PEDOT:PSS solution. The optimized EtOH-based PEDOT:PSS solution exhibited conformal and uniform coating, with ultrathin nanocoated films obtained on a hydrophobic pyramid polydimethylsiloxane (PDMS) surface. The fabricated pressure sensor showed high performances, such as high sensitivity (−21 kPa−1 in the low pressure regime up to 100 Pa), mechanical stability (over 10,000 cycles without any failure or cracks) and a fast response time (90 ms). Finally, the proposed pressure sensor was successfully demonstrated as a human blood pulse rate sensor and a spatial pressure sensor array for practical applications. The solvent exchange process using ultrafiltration for these applications can be utilized as a universal technique for improving the coating property (wettability) of conducting polymers as well as various other materials.


Flexible pressure sensors that can transform the physical sense of pressure into meaningful information through a capacitive, resistive, or piezoelectric medium have gained substantial attention due to the significant findings for various promising applications, including rollable touch displays, artificial electronic skin, robotics, and healthcare monitoring1,2,3,4. Promising routes to improve the sensor performance in terms of good mechanical stability, high sensitivity, high response time, and robustness through newly emerged advanced functional materials have been demonstrated in recent years. Based on various sensing mechanisms, resistive-type pressure sensors have been widely reported to provide additional functionalities to the sensor. Microstructures of elastomer materials have been the key factor in providing rubber-like elastic mechanical behavior to these sensors. However, elastomer materials are hydrophobic, and it becomes difficult to deposit uniform and adherent films of conductive materials. Moreover, the situation becomes worse on uneven surfaces. Although conductive materials, such as metals, can be deposited uniformly over large areas, they are brittle and difficult to apply to flexible devices. Therefore, materials possessing flexibility, high conductivity and good wettability are essential. In this respect, conducting polymers are very suitable due to the characteristics of high flexibility, good conductivity, large area, mass producibility, solution processability, and so on5,6,7,8,9,10,11,12. PEDOT:PSS was chosen for this work because it has the highest conductivity among various conducting polymers. However, commercialized PEDOT:PSS with high conductivity is dispersed in water, so the ability of the water-based PEDOT:PSS solution to coat on hydrophobic elastomeric substrates is limited due to the insufficient wettability of the aqueous solution. Thus, to provide uniform and adhered films, either the substrates undergo various surface treatments to facilitate hydrophilicity or wetting agents (e.g., the Zonyl surfactant) are added to the water-based PEDOT:PSS solution to provide good wettability. In either of these cases, there is always the possibility that the substrate will become oxidized, and the original characteristics will be modified or damaged. In the case of surfactants, the Zonyl surfactant in particular was registered as a regulated material under international regulatory policies, in which perfluorooctane sulfonate and perfluorooctanoic acid containing substantial amounts of fluorine atoms may lead to health issues; therefore, its production was discontinued in 201513,14,15. To overcome this issue, solvent exchange can be a good alternative because the contact angle with a hydrophobic substrate is lower in organic solvents than in water, resulting in better wettability. Several studies have reported exchange of water-based PEDOT:PSS solutions to organic solvents16,17,18,19. Despite the methods being attractive, the previous results exhibited low conductivity of PEDOT:PSS and involved limited solvents with high b.p. only; thus, the processing is very complicated, and the production scale is insufficient. The limitations pertaining to these methods are presented in Table 1. Therefore, it is highly essential to find a simple and proper way to improve the coating property without deteriorating the intrinsic properties of the PEDOT:PSS material.

Table 1 Previously reported solvent exchange processes for water-based PEDOT:PSS solutions.

Herein, we propose a facile way to greatly enhance the coating property of the PEDOT:PSS polymer on hydrophobic substrates using a solvent-exchange ultrafiltration method, presenting a solution to all the aforementioned concerns. The method not only exchanges solvents with high b.p. but also solvents with low b.p., such as volatile solvents (alcohols), while retaining the high conductivity of pristine PEDOT:PSS. In addition, the solvent exchange process is fast, universal, and easy to mass produce. Once PEDOT:PSS is dried in a solid state, it does not redisperse back into a solvent in its original state due to coagulation. Therefore, the solvent exchange process was designed to maintain the wet state of PEDOT:PSS until the end to avoid coagulation of PEDOT:PSS for good redispersion in organic solvent. Overall, the EtOH-based PEDOT:PSS solution made by this solvent exchange process exhibited excellent wettability on a hydrophobic PDMS substrate with a micropyramid array compared to other solvents without any additional surfactant. The pressure sensor fabricated using this approach exhibited high sensitivity in the low-pressure regime (−21 kPa−1, <100 Pa) possessing an exceptional uniform and conformal coating without any discontinuity, which is not the case with the water-based PEDOT:PSS. Moreover, the sensor was robust to extreme loads of cyclic mechanical behavior over 10,000 cycles without any failure or crack formation and had a fast response time of 90 ms, with a maximum load of 1 kPa. The pressure sensor was successfully demonstrated as a human blood pulse rate sensor and a spatial pressure sensor array. The highly conductive solvent-exchanged PEDOT:PSS developed in this study could facilitate new opportunities for flexible electronic devices, and the approach could be implemented as a universal technique for solvent exchange of various materials.

Materials and methods

Solvent exchange process for PEDOT:PSS solutions

A novel PEDOT:PSS solvent exchange process was carried out in a closed laboratory environment. Initially, a water-based PEDOT:PSS solution (Clevios PH 1000, Heraues) and an organic exchange solvent (1:1 volume ratio) were loaded in a lab-made filtration tank. Then, rotation and ultrafiltration processes were started simultaneously. The ultrafiltration was maintained at a pressure of 4–5 bar by an air-pressure pump. Regenerated cellulose membranes (nominal molecular weight limit: 10 kDa) were used for this ultrafiltration. The hydrophilic, tight microstructure of the membrane ensured the highest possible permeability with the lowest possible adsorption of PEDOT:PSS gel particles. Once the solvent was exchanged by a factor of 50%, another equivalent amount of solvent was added. This cyclical process was repeated 5–6 times until the solvent exchange ratio was 95% or higher.

Preparation of a PDMS substrate with a micropyramid array

Initially, a silicon mold was prepared using standard conventional photolithography procedures, as reported previously20. Then, the Si mold surface was cleaned and treated with a 3-amino-propyl triethoxysilane (99%, Sigma-Aldrich) solution to facilitate the formation of a thin hydrophobic layer for easy removal of the PDMS layer. Pouring the PDMS mixture (base:curing agent = 10:1) on the mold followed by exposure to vacuum allowed PDMS microstructures to form without any bubbles. Later, a flexible polyimide film was placed over the PDMS mixture and pressed with a known weight to promote the desired PDMS thickness throughout the experiments, which was followed by curing at 100 °C for 20 min, enabling the formation of 3D microstructures that were elastic in nature. Finally, a pyramid PDMS array was obtained by slowly stripping the film off the silicon mold.

Preparation of solvent-exchanged PEDOT:PSS films on the micropyramid array

The PDMS substrate with the micropyramid array was treated with O2 plasma for 3 min. Then, the solvent-exchanged PEDOT:PSS solution with EtOH as a solvent was mixed with 5 wt% dimethyl sulfoxide (DMSO) (99.9%, Sigma-Aldrich) to enhance the conductivity and diluted twice with EtOH (99.9%, OCI Company Ltd.) to ensure uniform thin film formation. The mixture was stirred and sonicated for 30 min and 2 min, respectively, followed by filtration through a 5.0 µm nylon syringe filter. Then, the mixture was drop-cast over the pretreated PDMS surface, with the excess solution removed by tilting the substrate vertically. Later, the sample was annealed in a convection oven at 150 °C for 15 min. The size of the sample with the micropyramid array was 1.5 cm × 1.5 cm.

Fabrication of a resistive pressure sensor device

The PEDOT:PSS film coating the PDMS pyramid array and Au-deposited PET film served as the bottom and top electrodes. Then, external wires were connected to the top electrode with the aid of anisotropic conductive film (ACF) bonding, while the bottom electrode was attached to the PEDOT:PSS coating with silver paste. Next, the top Au-coated PET film was placed and aligned over the PDMS microstructure, with the electrodes facing each other to further carry out electrical and mechanical characterizations.

Characterization and measurement

X-ray photoelectron spectroscopy (XPS) was performed with a K-alpha spectrometer (Thermo Fisher Scientific Inc.). Atomic force microscopy (AFM) and scanning electron microscopy (SEM) with energy dispersive X-ray (EDX) spectroscopy images were obtained using a Nanoscope Multimode Iva (Bruker Corp.) and a JEOL JSM-6710F field emission scanning electron microscope, respectively. The conductivities of PEDOT:PSS films were calculated based on their sheet resistance and thickness. The pH values of solvent-exchanged PEDOT:PSS solutions were measured using an MP-220 pH meter (Mettler-Toledo AG 8603 Schwerzenbach, Switzerland). The contact angles (CA) of PEDOT:PSS solutions were measured by a CA measuring device (Phoenix 300, South Korea). In the CA test solutions, 5% DMSO or 1% wetting agent (Capstone FS-30, Chemours Co.) was added to the PEDOT:PSS solutions with water and EtOH solvents, respectively. I–V measurements of the resistive pressure sensor device were carried out using a Keithley 4200-SCS semiconductor characterization system (Tektronix Co.). Pressure was applied or released by adding different loads to the device or removing them, respectively. The active area of the pressure sensor was 1.5 cm × 1.5 cm. For a touch panel array application, the solvent-exchanged PEDOT:PSS film coated on the PDMS pyramid array and the Au-deposited PET film were laser patterned by a programmable benchtop pulsed laser system (BasiCube 10, Scanlab Co.).

Results and discussion

Solvent exchange process using the ultrafiltration method

The important factor in solvent exchange of PEDOT:PSS is that PEDOT:PSS should remain wetted with the solvent to prevent coagulation of PEDOT:PSS. For this, a solvent exchange process using the ultrafiltration method was designed. Figure 1a shows the novel solvent exchange process (SEP) by ultrafiltration. The principle of this solvent exchange process is similar to changing cold water to hot water. Similar to adding hot water while removing cold water, an organic solvent well mixed with water is first added to aqueous PEDOT:PSS solution of the same volume. If half of the mixed solvent is removed through the membrane filter, then a solvent exchange ratio of 50% is obtained. In this mixture, half the volume is water, and the other half is the organic solvent. When this method is repeated 5–6 times, the solvent exchange ratio reaches 95% or higher. During this solvent exchange process, excess PSS or impurities can also be removed through the membrane filter at the same time. Figure 1b shows the dispersion stability of PEDOT:PSS solutions solvent-exchanged from water to various solvents after the SEP. EtOH and ethylene glycol (EG) were particularly selected as solvents for the solvent exchange of water-based PEDOT:PSS solutions because EtOH is widely used in alcohol organic solvents and EG is one of the most widely used conductivity enhancers of PEDOT:PSS. The dispersion stability was excellent in EtOH and EG, which can be explained by the Hansen solubility parameter. PEDOT and PSS have coulombic interactions with each other. The sulfonic acid of PSS is highly hydrophilic and dissociates into SO3 and H+ in water. Thus, PEDOT:PSS has excellent dispersibility in water due to the strong hydrogen bonding between the water molecules and SO3-. Supplementary Fig. 2a shows a graph of the Hansen solubility parameters of the solvents used in the SEP, indicating that the index determining the solubility is composed of three forces: the dispersion force (∂D), dipole–dipole force (∂P), and hydrogen bonding force (∂H)21,22,23. Supplementary Table S1 shows the values of ∂D, ∂P, and ∂H for each solvent. Among these three parameters, ∂H is mostly related to the dispersion stability of PEDOT:PSS. The higher the ∂H value of the solvent is, the better PEDOT:PSS is dispersed in the solvent, as shown in Fig. 1b. This relates to the mechanism by which PEDOT:PSS is dispersed in the solvent. PEDOT and PSS are connected by coulombic interactions, and PEDOT:PSS can be dispersed in solvent by the hydrogen bonding force between PSS and the solvent. Therefore, the higher the ∂H value of the solvent is, the stronger the hydrogen bonding force between the solvent and PSS, so PEDOT:PSS can be more stably dispersed in a solvent with a high ∂H value. Through our solvent exchange process, it has been confirmed that PEDOT:PSS was very well dispersed in a solvent with a ∂H value of 19.4 or higher. The solvent exchange ratio and the conductivity without the addition of DMSO are presented in Fig. 2b. After five or more SEP steps, the solvent exchange ratio reached 95% or higher. Note that the conductivity increased from 0.94 to 250 S/cm (in EtOH) without the addition of DMSO as a conductivity enhancer. This conductivity enhancement is due to the better connection between the conductive PEDOT chains, as the PEDOT and PSS are segregated by polar solvents such as EtOH24,25,26. Since EG is a typical conductivity enhancer, it exhibits a high conductivity of 1108 S/cm, even without DMSO. After the addition of DMSO, the conductivity in the water, EtOH, and EG solvents reached similar maximum values (Table S2). This means that the main chain of PEDOT, which is primarily responsible for the conductivity, remains unchanged, even after the SEP. XPS analysis was performed to confirm the change in the ratio between PEDOT and PSS after the SEP. Supplementary Fig. 2c shows XPS spectra of S 2p of PEDOT:PSS films from the water, EtOH, and EG solvents. The PEDOT:PSS ratio decreased from 1:2.37 in water to 1:1.90 in EtOH and 1:1.82 in EG, demonstrating the effect of removing the residual PSS in water. As the highly acidic PSS was removed, the pH of the PEDOT:PSS solution increased from 2.4 in water to 4.5 in EtOH and 4.4 in EG (Supplementary Table S2). Since the degradation of the atmospheric stability of PEDOT:PSS is mainly due to the hygroscopic property of PSS27, the reduction of the excess PSS can improve the atmospheric stability of PEDOT:PSS. Thus, the atmospheric stability of PEDOT:PSS depending on the solvent of PEDOT:PSS was analyzed by measuring the sheet resistance over time when exposed to air (temperature: 25 °C, relative humidity: 30%). The sheet resistance of the aqueous PEDOT:PSS increased by 98% on day 7, while the sheet resistance of EtOH- or EG-exchanged PEDOT:PSS increased by 38 or 34%, respectively. In other words, the atmospheric stability of solvent-exchanged PEDOT:PSS was improved by nearly three times compared to the aqueous PEDOT:PSS due to the effect of removing excess PSS (Supplementary Fig. S1). Supplementary Fig. S2a, b shows SEM and AFM images, implying that the gel particles increase in size after solvent exchange and that the crystallinity is improved by the 3D network structure and π–π stacking. This phenomenon is particularly evident in EG and is similar to that in previous reported studies of PEDOT:PSS treated by polar solvents, including EtOH and EG28,29,30,31,32,33. The contact angles (CA) of PEDOT:PSS solutions depending on the solvent and addition of a wetting agent (WA) on PDMS are presented in Fig. 2d (Supplementary Table S3). Among all the CA measurements, the PEDOT:PSS solution with water as a solvent showed a large variation from 96.94° to 49.18°, while the PEDOT:PSS solution with the EG solvent showed ~14° less variation, and the PEDOT:PSS solution with the EtOH solvent exhibited a negligible change (~0.16°) after the addition of the WA at 1%. Although the PEDOT:PSS solution with water exhibited a lower CA after the addition of the WA (49.18°), the PEDOT:PSS solution with the EtOH solvent without the WA displayed an even lower CA, thereby avoiding the necessity of a WA for wetting the surface. Therefore, it is clear from Fig. 2d that the PEDOT:PSS solution with EtOH as a solvent without a WA exhibited better coating properties (lower CA) than the solutions with EG and water. It is noteworthy that only the solutions with water and EtOH were mixed with 5% DMSO, not the solution with EG, because EG itself is a conductivity enhancer.

Fig. 1
figure 1

a Novel solvent exchange process by ultrafiltration. b Dispersion stability of PEDOT:PSS in various solvents after SEP.

Fig. 2
figure 2

a Graph of Hansen solubility parameters of the solvents used in SEP. b Variation in conductivity without the addition of DMSO and solvent exchange ratio depending on the number of SEP cycles. c XPS spectra of S 2p and (d) contact angle of PEDOT:PSS for various solvents by SEP.

Fabrication and characterization of a pressure sensor based on EtOH solvent-exchanged PEDOT:PSS

A step-by-step pressure sensor fabrication process using solvent-exchanged PEDOT:PSS with EtOH as a sensing material is schematically illustrated in Fig. 3a. The corresponding multilayer design layout and the sensor attached to the wrist artery for blood pulse monitoring are presented in Fig. 3b. A schematic illustration of the circuit model of the sensor mechanism with and without pressure is shown in Fig. 3c, where R1 and R2 represent the resistance before and after pressure is applied, respectively. To ensure PDMS microstructure formation, SEM measurements were performed, and corresponding images were obtained (Supplementary Fig. S3a–d). It was concluded that all pyramidal microstructures form sharp edges at the top without any structural deformation. To ensure a uniform coating of PEDOT:PSS on the uneven microstructure, drop-casting was preferred instead of spin-coating, which led to a nonuniform coating. As a systematic study, initially, pristine PEDOT:PSS solvent-exchanged with EtOH without dilution was used as prepared, without any additional changes. In this case, the SEM images showed thick coatings with a nonuniform thickness over the pyramids, as shown in Supplementary Fig. S4a,b. To obtain a more uniform and thin coating, the pristine solution was diluted twice with the same solvent (EtOH). Uniform and conformal nanocoating of PEDOT:PSS on the uneven surface without any agglomeration was observed, which is essential for practical applications (Fig. 4c, d). To further investigate the nanolevel thickness, uniformity, and presence of the PEDOT:PSS coating over the pyramids, SEM and EDX measurements were performed. As expected, due to the inclined surface, the thickness profile from the base to the top of a pyramid decreased from 90 to 10 nm according to cross-sectional SEM images, as shown in Fig. 4e–i. Similarly, the presence of the PEDOT:PSS coating was confirmed by EDX at the respective positions shown in Fig. 4e, f, h and Supplementary Table S4. The conformation and particle size (≈30 nm) of PEDOT:PSS are consistent with previous studies34,35. Notably, sharp edges with a uniform and conformal coating were observed at the top of the pyramids (also confirmed by EDX), as shown in Fig. 4h, which are crucial for minimizing large resistance deviations in response to pressure in the low pressure regime. On the other hand, commercial water-based PEDOT:PSS partially coated near the edge of the PDMS structure, leading to poor sensing performance (Figs. 4a, b and 5b). This can also be seen in Fig. 2d; the water-based PEDOT:PSS solution exhibited a high CA compared to the EtOH-based solution.

Fig. 3
figure 3

a Pressure sensor fabrication process using PEDOT:PSS solvent-exchanged with EtOH. b Overview of the fabricated pressure sensor. c Circuit model of the pressure sensor mechanism without and with pressure.

Fig. 4: SEM images of PEDOT:PSS coated on PDMS with pyramid arrays.
figure 4

ab Water-based PEDOT:PSS. cd PEDOT:PSS solvent-exchanged with EtOH. ei Cross section views of the thickness profile of PEDOT:PSS solvent-exchanged with EtOH from base to top (red, yellow, green, and blue) with EDX measured positions.

Fig. 5
figure 5

a, b Pressure sensitivity in the linear and saturation regime and (c) Response time of the proposed pressure sensor using PEDOT:PSS solvent-exchanged with EtOH. d Mechanical stability over 10000 cycles. Application of the pressure sensor to measure the human pulse wave (eg) Sensor wrapped on the wrist of the hand, blood pulse rate measured and pulse showing systolic and diastolic phase. hj Pressure sensor array demonstration.

The PEDOT:PSS solvent-exchanged with EtOH (diluted twice with EtOH) coating the PDMS pyramidal microstructure array was considered as a sensing material for the other electrical and mechanical characterizations. I–V measurements were carried out by applying a voltage across the two (top and bottom) electrodes such that a current flowed from the flat PEDOT:PSS substrate to the flat Au substrate through the pyramid tops. As pressure was applied to the top electrode, the pyramidal structures deformed, thereby increasing the contact area and, as a result, decreasing the resistance. Further increasing the pressure led to a negligible change in resistance due to the limited deformation of the pyramid microstructures. Conversely, as the pressure was decreased, due to the elastic nature, the PDMS structure tended to return to its original position, causing the resistance to increase. Figure 5a, b presents the sensitivity of the proposed pressure sensor, defined as S = (ΔR/R0)/ΔP, where ΔR is the change in resistance under applied pressure P, and R0 is the initial resistance under zero pressure. In the case of water-based PEDOT:PSS, the sensor showed poor sensitivity with large hysteresis, which is unfavorable for pressure sensing applications. In contrast, the sensor with PEDOT:PSS solvent-exchanged with EtOH (diluted twice with EtOH) showed high sensitivity with excellent reliability upon the increase and decrease (from 0 to 1 kPa and 1 kPa to 0 Pa) of pressure, almost retaining the original values when the pressure was removed, as shown in Fig. 5b. The plot exhibited two distinct pressure sensitivity regimes, one for low-pressure values <100 Pa, with a sensitivity S1 of −21 kPa−1, and the other for medium pressure values of 0.1–1 kPa, with a sensitivity S2 of −0.016 kPa−1. Note that the PEDOT:PSS solvent-exchanged with EtOH is not coated thinly and uniformly without dilution, and the pressure sensitivity is very poor, with a sensitivity S0 of −0.0001 kPa−1 (Supplementary Figs. S4, S5). The performance of the proposed sensor was compared with that of other sensors reported in the literature, as summarized in Supplementary Table S536,37,38,39,40,41,42,43,44,45,46,47. Although a few reports demonstrate very high sensitivities >20 kPa−1, the procedures to fabricate these sensors are very complex, and the structures obtained by nonconventional techniques are inadequate for producing reliable and repeatable data. Depending on the designed parameters of the microstructures, such as the shape, width, height, and spacing, the sensitivity and pressure regimes vary20,47,48,49. Our sensor showed a fast response time of only 90 ms, with a maximum load of 1 kPa, which is essential for practical pressure sensor applications (Fig. 5c). Figure 5d presents the mechanical stability of the pressure sensor using PEDOT:PSS solvent-exchanged with EtOH. Even after applying a cyclic pressure of 0.3 kPa for 10,000 cycles, the sensor exhibited high mechanical stability without peeling-off or resistance change.

Application of the proposed pressure sensor

Figure 5e–g presents the blood pulse and pressure sensor array applications of the proposed pressure sensor. To demonstrate a blood pulse rate sensor, the sensor was fabricated by laminating the PEDOT:PSS-coated PDMS microstructures with face-to-face alignment of the Au-coated PET sheet, followed by extracting external wires from the edges of the films with the aid of ACF bonding. Among various vital signs of the human body, the pulse is considered a primary vital sign of the human body to prevent cardiac diseases. The proposed pressure sensor attached to a wrist showed pulse waveforms in real-time monitoring, with a pulse frequency of 78 beats/min, which corresponds to that of a healthy adult. Moreover, the sensor exhibited distinguishable systolic and diastolic phases with P1, P2, and P3 peaks indicating incident, systolic, and diastolic waves4. Furthermore, Fig. 5h–j shows a 4 × 4-pixel array pressure mapping panel that enabled spatial resolution of the pressure. Figure 5h shows the multilayer structure of the array sensor. The PEDOT:PSS-coated pyramidal PDMS structure was patterned by a benchtop programmable nanosecond pulse laser to form four electrodes side-by-side in a row. Similarly, the Au-coated PET was also patterned to form four electrodes in a column (Supplementary Fig. S6). The four formed electrodes were connected to external wires with the aid of ACF bonding, while the patterned PEDOT:PSS layer was connected with silver paste. Then, the array sensor was sandwiched by attaching the top electrodes perpendicular to the bottom electrodes. The load of 0.6 g corresponded to 1.5 kPa applied to the second row and third column of the sensor array, and the difference in the applied pressure of the pixel was observed via the increased magnitude of the resistance, presented in Fig. 5h, i. Simultaneously, the spatial pressure distribution on pixels other than the applied pressure pixel exhibited a lower magnitude, thereby enabling precise localization of the applied load. This demonstrates the viability of the proposed pressure sensor for obtaining spatial pressure distributions.


Herein, highly conductive solvent-exchanged PEDOT:PSS dispersed in EtOH or EG showed very stable and homogeneous solutions. The PEDOT:PSS solution with EtOH as a solvent showed better coating properties than water without any aggregates. Applying the EtOH-based conductive PEDOT:PSS solution coating on hydrophobic substrates, such as PDMS, avoids the necessity of wetting agents, such as surfactants that alter the original properties of the materials. The pressure sensor fabricated by nanocoating conductive solutions on pyramidal PDMS structures exhibited ultrahigh sensitivity with a stable sensing performance. Moreover, the blood pulse rate and pressure mapping array sensors produced here were very accurate and sensitive, enabling spatial resolution of pressure. The advantages exhibited by these physical and mechanical properties of the solvent-exchanged PEDOT:PSS on microstructures enable potential applications in human-machine interfaces.


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This research was supported by the Basic Science Research Program through the National Research Foundation of Korea (NRF) (2017R1A2B4009963, 2018R1D1A1B07048232, 2019R1I1A1A01059217, and 2020R1I1A1A01073884 funded by the Ministry of Education). The researchers also acknowledge the support of the Korea Institute of Industrial Technology (KITECH); Research Project of Core Technology for Industry Leading Manufacture (KITECH EO-20-0019) and Korea Evaluation Industrial Technology (KEIT) through the Industrial Strategic Technology Development Program (No. 10079571).

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J-J.L. and S-G. mainly performed the experiment and wrote the paper. B-J.L., S-J.K. and S-Y.K. supported the experiment. S-J.L. and S-K.K. managed and advised on this research.

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Correspondence to Sunjong Lee or Sunkook Kim.

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Lee, J.J., Gandla, S., Lim, B. et al. Alcohol-based highly conductive polymer for conformal nanocoatings on hydrophobic surfaces toward a highly sensitive and stable pressure sensor. NPG Asia Mater 12, 65 (2020).

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