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Intrinsically Stretchable Large-Area Pixelated Electrochromic Displays via Direct Photopatterning
KangSikKim1
SooYeonEom2
SeongHwanYang1
Jeong-WanJo3
FayongSun2
BeomjinJeong2,4
Myung-Jae-Lee1
Jong-WoongKim6,7
Yong-HoonKim6
JongS.Park2,4,8✉Email
SungKyuPark1✉Email
1Department of Intelligent Semiconductor EngineeringChung-Ang University06974SeoulKorea
2School of Chemical Engineering, Department of Organic Material Science and EngineeringPusan National University46241PusanKorea
3Electrical Engineering Division, Department of EngineeringUniversity of Cambridge9 JJ Thomson AvenueCB3 0FACambridgeUK
4Department of Organic Material Science and EngineeringPusan National University46241BusanKorea
5Convergence Research InstituteDaegu Gyeongbuk Institute of Science and Technology (DGIST)42988DaeguKorea
6Department of Semiconductor Convergence EngineeringSungkyunkwan University16419SuwonRepublic of Korea
7School of Mechanical EngineeringSungkyunkwan University16419SuwonRepublic of Korea
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Research Institute for Convergence of Biomedical Science and TechnologyPusan National University
Kang Sik Kima†, Soo Yeon Eomb†, Seong Hwan Yanga†, Jeong-Wan Joc, Fayong Sunb, Beomjin Jeongb,d, Myung-Jae-Leee, Jong-Woong Kimf,g, Yong-Hoon Kimh, Jong S. Parkb,d,i*, and Sung Kyu Parka*
a Department of Intelligent Semiconductor Engineering, Chung-Ang University, Seoul 06974, Korea
b School of Chemical Engineering, Department of Organic Material Science and Engineering, Pusan National University, Pusan 46241, Korea
c Electrical Engineering Division, Department of Engineering, University of Cambridge, 9 JJ Thomson Avenue, Cambridge CB3 0FA, UK
d Department of Organic Material Science and Engineering, Pusan National University, Busan 46241, Korea
e Convergence Research Institute, Daegu Gyeongbuk Institute of Science and Technology (DGIST), Daegu 42988, Korea
f Department of Semiconductor Convergence Engineering, Sungkyunkwan University, Suwon 16419, Republic of Korea
g School of Mechanical Engineering, Sungkyunkwan University, Suwon 16419, Republic of Korea
h Department of Semiconductor Convergence Engineering, Sungkyunkwan University, Suwon 16419, Korea.
i Research Institute for Convergence of Biomedical Science and Technology, Pusan National University
*Corresponding Authors.
Email addresses: skpark@cau.ac.kr (S. K. Park) and jongpark@pusan.ac.kr (J. S. Park)
Abstract
Electrochromic displays (ECDs) have gained increasing attention for various stretchable applications, offering voltage-controlled optical modulation with low power consumption. However, realizing ECDs that include stretchability with high-resolution pixelation remains challenging. Here, we present an unprecedented combination of materials and device architectures that enable intrinsically stretchable and highly pixelated ECDs via direct photopatterning. Central to this strategy is a stretchable and photopatternable electrochromic (EC) material, containing acrylate-substituted RGB viologens, that supports direct photopatterning with high mechanical durability. To facilitate more strategic device architecture, a stretchable reactive spacer layer and a pixel-defining layer were introduced, ensuring uniform electrical contact and improving mechanical integrity with minimized crosstalk, respectively. Leveraging the cooperative function of the developed materials and device structures, we implemented a fully stretchable 10 × 10 passive matrix ECD that exhibits RGB pixelated coloration and maintains stable electrochromic performance under strains up to 30%, with durability sustained over 1500 mechanical cycles.
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1. Introduction
The increasing demand for mechanically robust and highly deformable electronics, such as wearable systems and biomedical devices, has accelerated research into 3D free-form display technologies that can seamlessly act as interactive interfaces for dynamic, arbitrarily shaped surfaces16. These devices need to be lightweight, energy efficient, and intrinsically stretchable, enabling facile integration with the human body while ensuring reliable optical and mechanical performance711. Electrochromic displays (ECDs), which reversibly modulate color under low-voltage electrical bias, offer a compelling platform for such applications12,13. Their simple architecture, comprising an electrochromic (EC) layer sandwiched between two electrodes, supports low power consumption, broad material compatibility, and scalability to large-area fabrication14. Accordingly, ECDs have been explored in smart windows1519, health monitors2022, flexible displays2329, and adaptive camouflage3032. Although inorganic ECDs based on tungsten oxide (WO3) exhibit excellent cycling stability and rapid switching speeds, the intrinsic brittleness of WO3 presents major limitations for mechanically deformable displays. While hybrid structures incorporating WO3 with flexible conductors, such as silver nanowires (AgNWs)29,33,34, offer improved durability, further integration with resilient EC materials remains challenging for the realization of full-color and high-resolution stretchable ECDs.
Organic-based ECDs offer a promising alternative due to their inherent flexibility and straightforward device configurations35. Various efforts to develop deformable devices have involved blending electrochromic polymers with elastomers, including those based on thiophene and phenylenevinylene18,19,29,30. Although these materials allow flexibility and durability, their limited patternability is still problematic for highly defined devices and pixelated display applications. As an alternative approach, viologen derivatives, 1,1’-substituted-4,4’-bipyridinium salts, have been incorporated into photocurable polymer matrices to fabricate flexible ECDs with reversible color switching25,26,36. However, these systems often suffer from poor interfacial contact between electrodes and EC layers, resulting in incomplete pixel activation, non-uniform coloration, and limited optical performance. To integrate highly defined ECDs in fully stretchable electronics, the devices must simultaneously exhibit photo-patternability, stretchability, and multicolor capability. Direct photopatterning is essential for achieving pixel-level definition and scalable integration; however, it remains extremely challenging to implement on stretchable, multilayered substrates due to issues such as optical scattering that hinders photopolymerization, mechanical mismatches between layers, and alignment distortions during processing.
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Here, we report the strategy for integration of materials and device architectures that enables intrinsically stretchable, highly photopatternable, and large-area pixelated ECDs. One of the key components for this system is a stretchable and photopatternable electrochromic (SPEC) material, developed by incorporating acrylate-substituted viologens into EC gels. The SPEC formulation comprising acrylate-functionalized viologens, an anodic EC component, an ionic liquid, and a photocurable elastomeric matrix, enables red (R), green (G), and blue (B) coloration with sub-micrometre resolution and mechanical resilience. Devices fabricated with SPEC materials demonstrate excellent EC stability, maintaining consistent coloration over 12,000 seconds of repeated cycling without performance degradation. Fine-patterned pixelation is directly achieved on highly stretchable polyurethane acrylate (PUA) substrates via ultraviolet (UV) irradiation, demonstrating sub-micrometre shapes.
For the facile implementation of fully stretchable ECDs, we further introduce two key architectural components: a stretchable reactive spacer layer (SRSL) with ion-gel and a pixel-definition layer (PDL) to enhance contact between deformable nanomeshed electrodes and the resilient SPEC materials, and structural integrity among the device components and less cross-talk in pixelated ECDs. Thus, the multicolor, pixelated ECDs exhibits stable and uniform color transitions under strains of up to 30%, maintaining durability over 1500 mechanical cycles, and significantly outperforms previously reported stretchable electrochromic systems. These findings underscore the synergistic importance of the SPEC material platform and the engineered SRSL and PDL architecture, providing a robust and scalable route toward high-definition, intrinsically stretchable ECDs that are compatible with standard CMOS processes.
Results
The ECD structure and the constituent components of the SPEC gels are illustrated in Fig. 1a-1c. In the stretchable ECD, the photo-patterned SPEC gel, integrated with SRSL and PDL, is sandwiched between two stretchable networked electrodes. Although the bottom electrodes and SPEC layer establish a highly conformal and reliable contact, mainly due to the bottom-up fabrication process where the SPEC is spun over the bottom electrodes, the top electrodes merely contact the SPEC layer, resulting in poor interfacial contact and weak adhesion. The SRSL and PDL are strategically introduced to ensure both stable electrical properties and mechanical durability of the ECD under extreme operating conditions. As shown in Fig. 1b, the SRSL provides a reliable and uniform electrical contact by eliminating the air gaps between the top electrodes and EC layer, while the PDL, which physically (electrically) separates the pixels, enhances mechanical integrity and prevents electrical crosstalk. The SPEC gel formulation comprises an acrylate viologen, PUA, diphenyl(2,4,6-trimethylbenzoyl)phosphine oxide (TPO), and 1,1'-dimethyl ferrocene (DMFc), combined with acetone, propylene carbonate (PC), and ionic liquids ([EMIM][TFSI] or [BMIM][TFSI]) (Supplementary Fig. 1). The RGB acrylate viologens displayed sufficient solubility in both ionic liquids, highlighting their suitability as media for SPEC gels. The use of ionic liquids was carefully guided through EC performance evaluations (Detailed explanation is provided in Supplementary Table 1–4 and Supplementary Note 1–4). PUA and TPO served as a UV-curable polymer matrix and photo-initiators, respectively. DMFc served as an anodic species, effectively suppressing undesired reactions between solvents and electrolytes, thereby reducing the operating voltage of ECDs by facilitating electron transfer during electrochemical reactions.
Fig. 1
Acrylate-substituted viologen-based SPEC gels for stretchable and multi-color ECDs.
a, Schematic of intrinsically stretchable, photo-patterned multi-color ECDs. b, Schematic of the cross-section of an intrinsically stretchable multi-color display. c, Schematic of chemical structure and compositions of SPEC gels. d-e EIS plot (d) and ionic conductivity (e) of SPEC-R, SPEC-G, SPEC-B, f, stress-strain curves of red, green, blue-color SPEC gels. g, photographs of red, green, blue SPEC gels: Initial state (top) and stretched state (bottom). h, Optical microscopy images of photo-patterned SPEC gels
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Red, green, and blue-color SPEC gels were prepared using different acrylate viologen derivatives. The SPEC gel containing red viologen was designated as SPEC-R, and those with green and blue viologens were labelled SPEC-G and SPEC-B, respectively. As shown in Fig. 1d-1e, electrochemical characterization revealed high ionic conductivities of approximately 3.6, 5.05, and 7.2 mS/cm for the SPEC-R, SPEC-G, and SPEC-B, respectively. Also, the Nyquist plots confirm stable charge-transfer kinetics, consistent with their excellent electrochemical performance. Following complete photo-curing, the SPEC gels exhibited high stretchability with maximum strain tolerances of 154% (SPEC-R), 169.3% (SPEC-G), and 120.3% (SPEC-B), with corresponding elastic moduli of 2.54 MPa, 2.190 MPa, and 4.12 MPa, respectively (Fig. 1f). The strain-dependent behaviours (Fig. 1g), highlight uniform deformation across all three layers in both relaxed and stretched states, confirming their robust resilience under dynamic conditions.
More importantly, the SPEC layers can be directly patterned onto PUA substrates, as illustrated in Fig. 1h. This compatibility arises from their shared chemical composition, with both materials featuring methyl acrylate terminal groups. Upon UV irradiation, polymerization is initiated, and polymer chain mobility gradually decreases. Residual unsaturated groups facilitate the formation of strong covalent bonds between the two layers, leading to strong interfacial adhesion. To enhance UV patternability and improve chemical compatibility with the PUA-based substrates, acrylate-functionalized viologens were employed. This chemical modification enables rapid, UV-triggered radical polymerization, as confirmed by Fourier transform infrared (FTIR) spectroscopy (Supplementary Fig. 2a-2c). The resulting covalent interactions, mediated by polymerized acrylate groups, not only strengthen interfacial bonding but also enable the formation of sub-micrometre resolution patterns. This is achieved by selectively dissolving the unexposed EC gel in dimethyl sulfoxide (DMSO) during the development process. A more mediated fine-patterning process was carried out using an optimized EC gel thickness of 60 µm, which was determined based on a balance between ionic conductivity and optical modulation, as displayed in Supplementary Table 4–6 and Supplementary Fig. 3–5.
In the device, the SPEC-R/G/B layers are deposited onto poly(3,4-ethylenedioxythiophene) : poly(styrene sulfonate) (PEDOT:PSS)/AgNWs electrodes, where the AgNWs are partially embedded within the PUA matrix. Notably, the PEDOT:PSS network does not completely encapsulate the PUA/AgNWs interface, leaving portions of the methyl acrylate-terminated PUA surface exposed (Supplementary Fig. 6). This residual chemical reactivity enhances intrinsic interfacial cohesion, thereby reinforcing the structural integrity of the layered assembly. To elucidate the nature of the interlayer bonding, FTIR spectroscopy was employed to analyze the chemical interactions between SPEC and PUA, with a focus on the acrylate functional groups (Supplementary Fig. 6a-c). For the SPEC/PUA sample, the PUA was partially cured to retain acrylate double bonds before deposition and complete curing of the SPEC layer. This sequential curing allowed additional covalent bonding between SPEC and the residual acrylate groups in PUA. FTIR spectra of individual SPEC and PUA layers, compared to the combined SPEC/PUA layer, revealed distinct spectral changes—most notably a peak at 1639 cm− 1—indicative of new covalent bonds formed at the interface. This interaction, driven by the shared methyl acrylate, substantially improves the cohesion between the layers. To quantitatively evaluate the adhesive strength of the SPEC layers, peel tests were conducted using various substrate configurations (Supplementary Fig. 6d). Polydimethylsiloxane (PDMS)- and polystyrene-block-poly(ethylene-ran-butylene)-block-polystyrene (SEBS)-based substrates exhibited immediate delamination, whereas thermoplastic polyurethane (TPU) substrates showed partial delamination and possible interfacial recombination via hydrogen bonding. PEDOT:PSS on PUA substrate showed higher adhesion, while PUA substrate exhibited a stable force throughout the displacement range, underscoring the exceptional interfacial bonding between SPEC and PUA. Furthermore, FTIR spectroscopy examined whether methyl acrylate groups facilitate covalent bonding between the electrode and SPEC in the presence of PEDOT:PSS and AgNWs. (Supplementary Fig. 6e-g). The SPEC layer was cured entirely on both AgNWs/PUA and PEDOT:PSS/AgNWs/PUA sides, evidenced by reduced at 1639 cm− 1 FTIR spectra. This result confirms the successful formation of covalent bonds, as the AgNW network, which was well embedded in the PUA, did not interfere with the bonding process. Consequently, the chain-like morphology and thus incomplete encapsulation of PEDOT:PSS is not likely to prevent direct covalent linkage between SPECs and PUA. These results collectively demonstrate that acrylate crosslinking proceeds effectively across the interfaces, enabling the formation of a continuous polymeric network even in the presence of electrodes.
To evaluate the electrochemical properties of SPECs, cyclic voltammetry (CV) was performed using a sandwiched structure with indium tin oxide (ITO) glass electrodes (Fig. 2a-2c and Supplementary Note 5). The anodic/ cathodic peak currents showed a linear relationship with the square root of the scan rate, indicating a diffusion-controlled mechanism37. Incorporating ionic liquids improved ionic conductivity, enhancing the redox characteristics and enabling reversible color switching of SPEC-R, SPEC-G, and SPEC-B to reveal red, green, and blue colored states (Supplementary Fig. 7). In spectroelectrochemical analyses, SPEC-R initiated coloration at -1.3 V, exhibiting a prominent absorption peak at 515 nm (Fig. 2d and Supplementary Fig. 3j). The transmittance contrast (ΔT) between bleached and colored states was 85.2% at 470 nm and reached 90.2% at 515 nm. SPEC-G showed coloration starting at -1.4 V, characterized by strong absorption peaks at 620 nm (visible region) and 851 nm (near-infrared (NIR) region) (Fig. 2e and Supplementary Fig. 4j). The corresponding ΔT values were 69% and 82.2%, respectively, showing NIR absorption capability due to the extended absorption range of the four pyridinium groups38. SPEC-B demonstrated prominent absorption at 539 nm and 602 nm upon applying − 1.3 V, achieving a ΔT of 83% at 602 nm (Fig. 2f and Supplementary Fig. 5j). The color changes of these SPECs were quantitatively analyzed through color coordinates (Fig. 2g-2h). In the bleached state, the xy coordinates of SPEC-R, SPEC-G, and SPEC-B were (0.33, 0.35), (0.31, 0.34), and (0.30, 0.36), respectively, corresponding to pale yellow. Upon electrochemical activation via applied voltage, these coordinates shifted to (0.46, 0.34), (0.29, 0.40), and (0.31, 0.27), clearly representing red, green, and blue coloration, respectively.
Fig. 2
Characterization of RGB-color SPEC gels.
a-c, Cyclic voltammetry curves with different scan rates for the (a) SPEC-R, (b) SPEC-G, and (c) SPEC-B SPEC gels fabricated using ITO electrodes. Inset images show the peak anodic and cathodic current vs. square root of scan rate. d-f, The corresponding transmittance change curves with different applied potentials for (d) SPEC-R, (e) SPEC-G, and (f) SPEC-B. g, Photograph of an operating image of ECD with different colors (SPEC-R(top), SPEC-G(middle), SPEC-B(bottom)). h, CIE color coordinates of three ECDs at different color states. i, Optical density graph of three ECDs (SPEC-R(left), SPEC-G(middle), SPEC-B(right)) j, Kinetic stability of three ECDs obtained at different wavelengths corresponding to different colors (SPEC-R(top), SPEC-G(middle), SPEC-B(bottom)). k, In situ dynamic transmittance responses for the three ECDs obtained at different wavelengths corresponding to different colors (SPEC-R(left), SPEC-G(middle), SPEC-B(right)) under square-wave voltage between − 2 and 0.5 V.
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Fig. 3
PEDOT:PSS/AgNWs/PUA stretchable electrodes
(a) Schematic of the fabrication process for the PEDOT:PSS/AgNWs/PUA stretchable electrode. (b) SEM images of PEDOT:PSS/AgNWs/PUA stretchable electrode, (c) The SEM image (left) and EDS mapping for PEDOT:PSS/AgNWs/PUA : Ag(middle) and sulfur(right), and (d) The SEM images of AgNWs patterns with a line width of 10, 20, 30, 50, 100, 200, 250 and 500 µm(left). The high magnification SEM image of the AgNWs line pattern with a line width of 10 µm (right). (e) AFM image of PEDOT:PSS/AgNWs/PUA stretchable electrode.
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Alternating voltages of -1.5 V and 0.5 V were applied in 20-second intervals to evaluate the stability and coloration efficiency (CE) of the ECDs (Fig. 2i-2k). The CE, a key figure of merit, relates optical modulation to the charge involved in the redox process, and was calculated as
where
is the exchanged charge density and
, with
​ and
denoting transmittance in bleached and colored states.
Initially, SPEC-R showed a ΔT of 83.1%, slightly decreasing to 78.9% after 5 cycles. Within the first 30 cycles, Tmin increased from 1.2% to 5.4%, stabilizing at 3% after 300 cycles (12,000 s), while maintaining a ΔT of 75.2%. The CE for SPEC-R was 52.0 cm2/C, with estimated coloration (τc) and bleaching (τb) switching times of 17 and 11 s, respectively. Moreover, SPEC-G exhibited a ΔT of 69.2%, which reduced to 54.7% after 300 cycles, representing a CE of 289.3 cm2/C and switching times of 6 s (τc) and 4 s (τb). SPEC-B maintained a ΔT of 82.4% over 300 cycles with a CE of 253.5 cm2/C, and the switching times (τc and τb) of 18 and 9 s.
Fig. 4a
shows the structure of intrinsically stretchable ECDs composed of SPEC and PEDOT:PSS/AgNWs composite electrodes. The colored and bleached states of SPEC-R, SPEC-G, and SPEC-B at 60 µm SRSL thickness are depicted in Fig. 4b, confirming successful ECD operation. SRSL thickness was determined based on stable operation and stretchability (Supplementary Fig. 11). To investigate the SPEC properties, the redox behaviors of SPEC-R, SPEC-G, and SPEC-B were evaluated using CV measurement (Supplementary Fig. 12a-12c). The observed redox behaviours were comparable to those of ECDs fabricated with ITO electrodes. Coloration for red, green, and blue was initiated at -1.4 V, -1.3 V, and − 1.3 V, respectively, with all devices demonstrating operating voltages less than − 2 V. These characteristics suggest favourable compatibility between the stretchable electrodes and SPECs, ensuring reliable voltage delivery and thus stable and energy-efficient EC performance. Additionally, the devices exhibited a linear dependence on the square root of the scan rates for both anodic and cathodic peak currents, consistent with a typical one-electron transfer process described by the Randle-Sevcik Eq. 43.
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The equivalent circuit of the stretchable ECD is illustrated in Fig. 4c, where Re represents the resistance of the stretchable electrodes, Rct denotes the charge transfer resistance, Zw corresponds to the Warburg impedance, and Cdl signifies the double-layer capacitance. Under direct current bias, Cdl behaves as an open circuit, allowing the equivalent resistance (Req) to be expressed as Req = 2(Re + Rct + Zw). Notably, all of these resistive components are highly strain-sensitive. In stretchable electrodes, resistance typically increases in proportion to the square of the applied strain. Similarly, our AgNW-based composite electrodes exhibit a severe increase in resistance with strain, primarily due to the percolation-dependent nature of randomly distributed AgNW networks (Fig. 4c). This increased resistance directly impacts device operation by reducing the voltage drop across the SPEC layer, thereby limiting the effective bias available for electrochromic switching. Such phenomena typically introduce a critical hurdle to implementing strain-resilient, high-performance stretchable ECDs. However, the device architectures we proposed in this research can address these challenges throughout optimized electrode design and interface engineering, such as PEDOT:PSS integrated AgNWs and SRSL and PDL layers, which mitigate resistance growth under strain.
Fig. 4
Electrochromic properties of an intrinsically stretchable electrochromic ECD.
a, Device structure of the intrinsically stretchable ECD. b, Photographs of coloration and bleached state of intrinsically stretchable ECD. c, Schematic of the intrinsically stretchable ECD circuit (left), normalized resistance (R/R₀) under strain up to 50% for EC, SPEC gel, and PEDOT:PSS/AgNWs/PUA electrodes (right). d-h, Photographs of intrinsically stretchable ECDs stretched up to 50% for SPEC-R(left), SPEC-G(middle), and SPEC-B(right). g-i and j-l, Transmittance curves of intrinsically stretchable ECDs for SPEC-R, SPEC-G, and SPEC-B at 0 V and 1.5 V under mechanical strain from 0% to 50% (g-i) and after 0, 10, 100, 500, 1000, and 1500 stretching cycles at 30% strain (j-l).
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EC performance under mechanical deformation was evaluated, as shown in Fig. 4d-4f. The transmittance spectra and switching behaviours of red, green, and blue ECDs were measured under strains of up to 50%. In the bleached state, a slight increase in transmittance was observed with increasing strain, attributed to the expanded spacing within the AgNW network, which allows more light to pass through. In the colored state, a comparable increase in transmittance was observed, attributed to the strain-induced increase in resistance that reduces the effective coloration bias. Despite these optical variations, the devices maintained strong EC functionality. Even at 50% strain, the transmittance differences between the bleached (T0) and colored (Tcolor) states were 57.77%, 41.53%, and 49.57% for red, green, and blue ECDs, respectively—values that remain comparable to their pristine (0% strain) conditions of 42.35%, 43.54%, 46.85% (Fig. 4g-4i). To further validate mechanical robustness, we conducted fatigue tests involving 1500 stretch–relaxation cycles between 0% and 30% strain. The corresponding T0 - Tcolor values over these cycles are shown in Fig. 4j-4l. A slight decline in optical contrast was observed within the first 500 cycles, after which performance remained relatively stable. After 1500 cycles, the T0 - Tcolor values were retained at 40.36%, 51.40%, and 44.60% for red, green, and blue devices, respectively. These results demonstrate that the current ECDs not only survive but maintain functional integrity under sustained and challenging mechanical strain, highlighting the success of material and structural design strategies.
To realize highly pixelated stretchable ECDs, three SPEC gel arrays were photo-patterned onto a stretchable electrode substrate. Sub-pixelated ECDs were fabricated by sequentially patterning the SPEC gels through a drop-casting and UV-curing process, as illustrated in Fig. 5a. A critical consideration during the SPEC gel patterning process is avoiding exposure of the EC solution to oxygen, which inhibits the photopolymerization of acrylate-based resins44,45. Supplementary Figs. 13 and 14 show fabrication details and the PDL with SPEC pixels. The incorporation of PUA in both the SPEC gels and the electrode substrate also significantly enhanced the adhesion of the cured SPEC gels, contributing to robust structural integrity under deformation. The proposed device architecture implies three essential advantages: 1. Enhanced interfacial bonding. The SRSL ensures secure bonding between the top electrode and underlying layers. During UV curing, polymer chains form covalent bonds with adjacent layers, effectively integrating all device components into a cohesive assembly (Fig. 5b). 2. Enhanced electrical connectivity. The SRSL fills air gaps between the multi-layered SPEC pixels and the top electrode, enabling conformal electrical contact that facilitates efficient ion transport. This design leads to enhanced EC switching behaviours. To suppress signal crosstalk arising from ion diffusion in the SRSL, the PDL provides pixel confinement (Fig. 5c). All functional materials—stretchable electrodes, SPEC layers, SRSL, and PDL—are physically confined within defined pixel areas, eliminating undesired lateral diffusion. The mechanism is schematically illustrated in Fig. 5d. Notably, as shown in Fig. 5e, ECDs fabricated without the SRSL showed low and diminished current densities, indicating ineffective electrochemical contact and switching behaviours. In contrast, SRSL-integrated devices exhibited high and stable current densities, confirming reversible electrochemical reactions facilitated by robust electrical pathways. 3. Mechanical stress release. The SRSL and PDL also serve to redistribute mechanical stress across the device surface. Horizontal and vertical air gaps between SPEC sub-pixels and SPEC and electrodes, respectively, can be considered as zero modulus areas, resulting in significant modulus mismatch and localized stress concentration at pixel boundaries and electrode interfaces. This mismatch is a common cause of cracking or delamination under strain. Therefore, devices without the SRSL fractured immediately upon strain, whereas those with SRSL maintained electrical and mechanical stability up to 50% strain (Supplementary Fig. 12d-i). Finite element simulations (COMSOL) confirmed that placing the SRSL and PDL in these regions effectively redistributes stress, releasing the imposed stresses and thus preventing localized failure (Fig. 5f). This stress-balancing strategy allows the device to maintain structural cohesion and stable coloration performance even under substantial mechanical deformation. To ensure the scalability and practicality of the developed SPECs and device architectures, we implemented large-area pixelated passive matrix (PM) stretchable ECDs with 10 × 10 RGB pixels, verifying the efficacy of the materials and devices for high-quality stretchable applications. These free-standing, multicolor pixel arrays demonstrated excellent mechanical durability and reliable coloration for 1,500 mechanical strain cycles at strains up to 30%. (Fig. 5g-h and Supplementary Fig. 15). Notably, no degradation or crosstalk was observed between adjacent pixels under stretched states. All RGB colored characters and images were implemented, and full-pixel activation of blue arrays was successfully demonstrated.
Fig. 5
Structures and key components for large-area pixelated multicolor stretchable displays.
a, Schematic of the fabrication process of stretchable sub-pixelated multi-color ECDs. b, Schematic of the bonding process by UV curable SRSL. c, Schematic and photographs of the ion transport in the EC pixelated display: w/o PDL (left), w/ PDL (right). d, Schematic illustration of two stretchable ECDs: w/o SRSL (top), w/ SRSL (bottom). e, Current density curves of two stretchable ECDs : w/o SRSL (top), w/ SRSL (bottom). f, Schematic (left) and COMSOL simulation data at 30% strain (right) of the stress relief effect of PDL and SRSL at 30% strain. g-h, Photographs of stretchable sub-pixelated passive matrix ECD arrays (g) SPEC-R (left), SPEC-G (middle), and SPEC-B (right) under 30% strain; (h) RGB sub-pixels (top) and SPEC-B (bottom) under 30% strain.
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Discussion
In this article, we presented a general and scalable strategy for realizing highly pixelated intrinsically stretchable full-color ECDs that outperform the state-of-the-art stretchable counterparts. To address the above requirements, we proposed a novel material design and facile implementation methods based on direct photo-patternable acrylate-substituted viologens and PUA mediated stretchable electrodes. This approach is further integrated with ion gel-based stretchable components such as SRSLs and PDLs to achieve system-level robustness and scalability, validating significantly improved interfacial adhesion and overall device performance via CMOS-compatible processes. These intrinsically stretchable, high-resolution ECDs could be of use for a wide range of applications in large-area skin-worn displays, healthcare monitoring and professional outdoor platforms, offering a solid foundation for full autonomy of next-generation intrinsically stretchable electronic systems.
Methods
Materials
Raw material, imidazole, triphenylphosphine (PPh3), bromine, 2-hydroxyethyl acrylate, sodium bicarbonate (NaHCO3), 1,2,4,5-tetrabromobenzene, hydroquinone, 1,4-diiodobenzene, ammonium hexafluorophosphate (NH4PF6), lithium bis(trifluoromethanesulfonyl)imide ([Li][TFSI]), 1-ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide ([EMIM][TFSI]), 1-butyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide ([BMIM][TFSI]), diphenyl(2,4,6-trimethylbenzoyl)phosphine oxide (TPO), anhydrous dichloromethane, 1,4-dioxane, propylene carbonate were purchased from Sigma aldrich. 4-pyridienboronic acid, Potassium carbonate, Tetrakis(triphenylphosphine)-palladium(0), 4,4-bipyridine, ferrocene (Fc), magnesium sulfate (MgSO4) were purchased from TCI chemical. Methacrylate-polyhedral oligomeric silsesquioxane (MA-POSS) was purchased from Hybrid Plastics. Dichloromethane, petroleum ether, ethyl acetate, acetonitrile, methanol, dimethylformamide, and dimethyl sulfoxide were purchased from Daejung and used without any purification.
Synthesis of AC-R, AC-G, and AC-B viologens
The details of all synthetic procedures Synthesis of 4,4’-(1,4-phenylene)bis(1-(2-(acryloyloxy)ethyl)pyridin-1-ium) (AC-R), Synthesis of Synthesis of 4-(2,4,5-tri(pyridine-4-yl)phenyl)-bis(1-(2-(acryloyloxy)ethyl)pyridine (AC-B), Synthesis of 1,1'-bis(2-(acryloyloxy)ethyl)-[4,4'-bipyridine]-1,1'-diium (AC-G) are available in Supplementary Note I, Supplementary Figs. 1–3, Supplementary Table 4.
Preparation of the polyurethane acrylate precursor
A flask charged with polyol (25 g, 100 mmol) and Methyl ethyl ketone (MEK) (25 mL) was heated at 60 oC until the solution turned clear, after which Isophorone Diisocyanate (IPDI) (8.33 g, 150.0 mmol) and dibutyltin dilaurate (cat.) were added. This mixture was then heated at 60 oC for 3 hours, and after adding HEA (2.9 g, 99.9 mmol), it was stirred for an additional 3 hours at 60 oC before cooling to room temperature. It was then mixed with an Irgacure 184 at a ratio of 10:0.36.
Synthesis of SRSL
The polyurethane acrylate (6 g), [BMIM][TFSI] (1.5 g), [Li][TFSI] (1.5 g), ferrocene (Fc) (20 mg), TPO (216 mg), and 2-propanone (1.5 g) were mixed and stirred for 24 hrs at 80 oC.
Synthesis of PDL
The polyurethane acrylate (6 g) and Irgacure 184 (0.36 g) were stirred for 20 min at room temperature.
Fabrication process of stretchable electrodes
A dispersion of AgNWs in water (concentration of 1 mg ml− 1) was coated on bare wafer substrates using a #5 Meyer rod until sheet resistance was under 30 Ω/sq and annealed at 120 oC for 1 min. PEDOT:PSS ink was prepared for the electrode solution using PEDOT:PSS (1.3 wt% dispersion in water, Clevios pH 1000) (10 g). Then, DMSO (2.5 g) and glycerol (1 g) were added and stirred at room temperature for 2 hrs. After that, ethylene glycol (0.5 mL) and DBSA (0.05 mL) were added and stirred for 15 min. The prepared PEDOT:PSS solution was spin-coated on the AgNWs layer using a consecutive two-step coating process with different spin speeds (500 rpm, 10 s, and 1500 rpm, 20 s) and subsequently annealed at 120°C. The obtained transparent conductive coating on the wafer substrates was then coated with a PUA solution. The PEDOT:PSS and AgNW layers were patterned by conventional photolithography and wet etching with Cr etchant (ETCR-300). The PUA solution was spin-coated at 300 rpm for 60 s. The coated AgNWs wafer was placed in a convection oven at 80 oC for 1 hr to evaporate residual solvent and level the plane, then cured with a UV lamp. After that, the patterned electrodes were heated at 80°C for 1 hr and then immersed in water for 1 hr to peel off.
Fabrication of stretchable ECDs
Polystyrene (Sigma Aldrich average Mw~350,000) (25 g) and toluene (25 mL) were stirred for 12 hrs at 80 oC. The polystyrene solution was spin-coated on bare glass at 1000 rpm for 60 s, and then heated at 100°C for 10 min. Unpatterned PEDOT:PSS-AgNW-PUA composite electrodes were transferred to polystyrene-coated carrier glass. The EC solutions were drop-cast onto the composite electrodes and cured under UV irradiation (350 nm, 145 W) through a PDMS-coated glass, resulting in a final layer thickness of 60 µm. After curing, the PDMS glass was removed. The SRSL solution was drop-cast onto the SPEC gel/electrode surface. The second electrode was then aligned in reverse and placed on top of the SRSL-coated SPEC gel. UV light was applied through the second electrode to cure the SRSL solution in place. After curing, the assembled device was carefully removed from the carrier glass.
Fabrication of multi-colored stretchable ECDs
The SPEC gel solution was drop-cast onto a PEDOT:PSS-AgNW-PUA and cured by UV (352 nm, 15 W) irradiation through a PDMS layer. The UV curing times of red, green, and blue SPEC gels were optimized at 180 sec. The uncured SPEC gel, not exposed to the UV light during the developing process, was developed by washing with acetone and deionized water. Then, the SPEC gels were pixelated onto the stretchable electrode.
The PDL solution was drop-cast onto the pixelated SPEC gels and stretchable electrode, then the structure was flipped and UV-cured through the PDMS layer. After that, the SRSL solution was drop-cast on the resulting substrate. Lastly, the second stretchable electrode was placed on top of the subpixelated SPEC gels. To cure the SRSL solution sandwiched between two electrodes, the UV light is exposed through the top electrode for 300 s.
Characterization and measurements
The ECD cells were fabricated by placing the prepared SPEC gel on an ITO-coated glass. The ITO-coated glass was sandwiched with a Surlyn film and measured in a two-electrode system using an SP-150 potentiostat (Biologic). Absorption and spectroelectrochemical measurements were performed using a UV-1800 UV–Vis spectrophotometer (Shimadzu). The kinetic stability of the ECDs was measured by applying constant potential stepping with a Biologic SP150 potentiostat, and the corresponding change in transmittance was monitored with a UV–Vis spectrophotometer. The percent transmittance (ΔT), the change in the optical density (ΔOD), and the coloration efficiency (CE) were calculated using the following relationships: ΔT = Tmax − Tmin, ΔOD = log Tb/Tc, and CE = ΔOD/Qd, respectively, where Tb and Tc indicate the bleached and colored transmittance values, respectively, and Qd is the injected charge per unit area. Tensile properties were also assessed using a Universal testing machine (UTM) under a constant strain-rate testing mode. Microstructures and surface morphologies of thin films were investigated by using optical microscopy (OM, BX53 M, Olympus), atomic force microscopy (AFM, NX10, Park-systems), and field emission scanning electron microscopy (FE-SEM, SIGMA 300, Carl Zeiss,), elemental composition profiles of the stretchable electrode were investigated using Energy Dispersive X-ray Spectroscopy (EDS) during the SEM analysis. For the dynamic measurement of the resistance of stretchable electrodes, a measurement system comprising a switch mainframe (Keithley 3706A), a double-channel source meter (Keithley 2636B), and a high-speed reed relay MUX card was used, connected to a data acquisition system (DAQ; SnM).
Finite element simulation
To investigate the stress distribution of pixels of the stretchable subpixelated ECDs and their relevant mechanisms, a numerical stress/strain analysis using FEA (COMSOL Multiphysics 5.3) was carried out. The cubic EC pixels were designed in the actual array size (720 mm [width] × 1 mm [length] × 60 mm [height]).
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Acknowledgements
This research was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea Government (MSIP) (No. RS-2024-00347845). This work was supported by the Nano & Material Technology Development Program through the National Research Foundation of Korea (NRF) funded by Ministry of Science and ICT(RS-2023-00281346). This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korea government (MEST) (RS-2023-00221396).
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Author contributions
S.K.P. and J.S.P conceived the idea for this work and designed the materials and experiments. K.S.K., S.H.Y and S.Y.E. synthesized EC materials, implemented intrinsically stretchable ECDs, and characterized all the data. J.-W.J,, B. J., M. -J. -L., J. -W. K., and Y. -H. K. provided suggestions for the experiment designs. S.H.Y., and F. S. assisted the characterization of materials and device properties. K.S.K., and S.H.Y conducted COMSOL simulation. K.S.K., S. Y. E., S.H.Y., J.S.P., and S.K.P. wrote the manuscript based on the input from all the authors. S.K.P., J.S.P., Y.H.K. and J.-W.K. reviewed and revised the manuscript. All the authors participated in discussions regarding the findings and collectively endorsed the manuscript.
Electronic Supplementary Material
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