Unlocking the Full Spectrum: A Paradigm Shift in Electrochromic Devices with High-Performance Black Conjugated Polymers

Unlocking the Full Spectrum: A Paradigm Shift in Electrochromic Devices with High-Performance Black Conjugated Polymers | Research Square window.SnipcartSettings = { analytics: { enabled: false } }; (function() { var accessVector = localStorage.getItem('access_vector') || ''; window.dataLayer = window.dataLayer || []; if (accessVector) { window.dataLayer.push({ user: { profile: { profileInfo: { snid: accessVector } } } }); } })(); (function(w,d,s,l,i){w[l]=w[l]||[];w[l].push({'gtm.start':new Date().getTime(),event:'gtm.js'});var f=d.getElementsByTagName(s)[0],j=d.createElement(s),dl=l!='dataLayer'?'&l='+l:'';j.async=true;j.src='https://www.googletagmanager.com/gtm.js?id='+i+dl;f.parentNode.insertBefore(j,f);})(window,document,'script','dataLayer','GTM-K279D39R'); Browse Preprints In Review Journals COVID-19 Preprints AJE Video Bytes Research Tools Research Promotion AJE Professional Editing AJE Rubriq About Preprint Platform In Review Editorial Policies Our Team Advisory Board Help Center Sign In Submit a Preprint Cite Share Download PDF Article Unlocking the Full Spectrum: A Paradigm Shift in Electrochromic Devices with High-Performance Black Conjugated Polymers Dinghui Chen, Zizheng Tong, Qiushi Rao, Hong Meng, Wei Huang This is a preprint; it has not been peer reviewed by a journal. https://doi.org/ 10.21203/rs.3.rs-3939829/v1 This work is licensed under a CC BY 4.0 License Status: Published Journal Publication published 30 Sep, 2024 Read the published version in Nature Communications → Version 1 posted You are reading this latest preprint version Abstract The black-to-transparent electrochromism is hailed as the "Holy Grail" of organic optoelectronics. However, designing black electrochromic (EC) materials that fully absorb in the visible light region remains challenging. Electroactive materials that simultaneously possess excellent cyclic stability, fast switching times, and high coloration efficiency are extremely rare. In this work, copolymers capable of fully absorbing across the entire visible spectrum have been successfully designed through judicious selection of four types of monomers. We introduce two types of polar side chains, which synergistically improve the ionic conductivity of copolymer, thereby enhancing the performance of electrochromic devices(ECDs). ECDs exhibit unprecedentedlong-term cyclic stability, surpassing all previously reported high cyclic stability devices with over 126,786 cycles. Additionally, they achieve a coloration efficiency of 1273 cm²/C, which exceeds that of every high coloration efficiency ECDs present so far, along with fast coloring/bleaching times of 0.82 s/0.86 s. This study presents a new strategy for the design and synthesis of high-performance black electrochromic copolymers. Physical sciences/Materials science/Materials for devices/Electronic devices Physical sciences/Materials science/Materials for optics organic optoelectronics black electrochromic materials transparent high stability coloration efficiency Figures Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Introduction Recently, the development of advanced EC materials has become a cornerstone that intertwines function with environmental sustainability. The core of this advancement is the design of EC materials, which have revolutionized the field due to their ability to undergo reversible optical transitions in response to electrical stimulus 1, 2 . These materials play an important role in the emerging field of smart technologies, such as energy-efficient displays, smart windows, and smart sunroof 3 , which are changing our lives. However, the widespread practical deployment of EC materials faces several significant obstacles, such as limited stability, slow switching times, and low coloration efficiency. To unlock its full potential, it is imperative to design EC copolymers with high performance that address these challenges. Black-to-transmissive EC materials are particularly eye-catching among EC materials. Black materials have the ability to absorb light almost completely, offering the possibility of improving energy efficiency in buildings and vehicles. However, the development of black ECDs still remains challenging task due to the complexity of broad absorbing spectrum modulation to cover the whole visible region homogeneously 4 . In their seminal work, Reynolds et al. developed copolymers using 2,1,3-benzothiadiazole (BTD) and 3,4-bis(2-ethylhexyloxy)thiophene (DOT-(OEtHx) 2 ), revealing limited absorption in the 420–550 nm range 5 ( Figure S1 a) . In their later work, they innovatively synthesized electrochromic polymers capable of transitioning from black to transmissive using a Stille polymerization approach with distannyl and distannyl 3,4-propylenedioxythiophene (ProDOT-(CH2OEtHx) 2 ), along with 2,4,7-dibromo-2,1,3-benzothiadiazole. While the absorption range improved, challenges persisted with insufficient intensity in the 360–480 nm range (Figure S1 b ) 6 . In parallel, Bao et al. utilized poly(3-hexylthiophene-2,5-diyl) (P3HT) in stretchable electronic skin, noting that the P3HT ECDs demonstrated relatively weak absorption in the 400–500 nm range under various stress conditions ( Figure S1 c ) 7 . Leveraging direct C–H arylation and Stille polymerization for synthesizing black materials garnered significant interest. Recently, a novel black polymer was synthesized using 3,3-bis((2-ethylhexyloxy)methyl)-3,4-dihydro-2H-thieno[3,4-b][ 1 , 4 ]dioxepine and 4,7-dibromo-2,1,3-benzothiadiazole monomers through a concerted metalation-deprotonation pathway 4 . Although its absorption in the 400–500 nm range remained suboptimal ( Figure S1 d ). Yan et al. explored this by integrating diverse spacing units such as carbazole, naphthalene, and phenylene into a ProDOT and BTD copolymer, yet observed a persistent weak absorption in the 400–500 nm spectrum ( Figure S1 e ) 8 . However, there is still a weak absorption of varying degrees in the 400–500 nm (Figure S1 e). Although alternative methods have been explored to develop black materials that can absorb all visible light, these attempts have not yet met the expected outcomes 5, 6, 9–19 . Up to now, synthesizing true black conjugated polymers remains a challenging frontier, as it demands precise control of the molecular structure, and requires a balance between broad-spectrum absorption, stability, and processability 6 . In the EC field, simultaneously achieving ultra-high stability, fast switching times, and high coloration efficiency in black EC conjugated polymers is a significant challenge 20–22 . Most materials only exhibit high performance in one or two parameters, and it is very rare to meet three parameters simultaneously 23–25 . This difficulty is primarily attributable to three major challenges. Firstly, conjugated polymers inherently exhibit low ionic conductivity. This limitation hinders the effective movement of ions, leading to a decrease in the overall performance of devices that incorporate these polymers. Secondly, the complexity of molecular design necessitates precise control over the structure, including monomer selection, polymerization methods, and chain arrangement, where enhancing one property may adversely affect others. Thirdly, the optimization of ECD properties involves inherent trade-offs: enhancing stability often necessitates more rigid molecular architectures, which can prolong the switching times; concurrently, improved coloration efficiency may demand more complex molecular structures, potentially compromising stability and increasing switching times. To address the above challenges, in this work, we strategically selected four types of monomers to design and synthesize high-performance EC materials. To address the limited absorption range of conjugated polymers in the visible spectrum, we introduced fluorene derivatives as additional monomers and simultaneously replaced the alkyl side chains of ProDOT with triethylene glycol (TEG) side chains to enhance the absorption properties of the copolymers. By adjusting the ratios of the four monomers, black copolymers were successfully synthesized. To tackle the challenges of limited stability, slow switching times, and low coloration efficiency in ECDs, we enhanced electronic conductivity by extending the conjugation lengths of four monomers, and introduced ester and TEG side chains into the copolymer to boost its ionic conductivity through the synergistic effect, thereby comprehensively improving the performance of ECDs. The bar-coating polymer thin film exhibited a deep black neutral state and attained transmissive state upon full oxidation. This work offers a novel strategy for designing high-performance black EC materials, laying the Results and discussion Properties of polymers Figure1. (a) Normalized UV-Vis solution absorption spectra of P1 polymers in chloroform solution (0.2 mg/mL); (b) Normalized UV-Vis solution absorption spectra of P2 polymers in chloroform solution (0.2 mg/mL); (c) Normalized UV-Vis solution absorption of Polymer P2-b in chloroform (0.25 mg/mL); (d) Energy level diagram of the P2 polymers;(e) P2 Coloration efficiencies efficiency. In the P1a-e polymer series, the concentration of monomer 1 was incrementally increased from 10 mol% to 90 mol%, while that of monomer 3 was correspondingly reduced from 90 mol% to 10 mol%. Figure 1(a) illustrates that the UV-Vis spectrum of P1-a features a pronounced absorption peak at 594 nm, accompanied by a less intense peak at 324 nm, resulting in a blue-colored solution. The spectrum of P1-b reveals a broad absorption peak at 596 nm and an additional peak at 366 nm. Moreover, upon adjusting the proportion of monomer 1 to 0.5 equivalents and reducing monomer 3 to 0.5 equivalents, a prominent new peak emerges at 404 nm, indicative of the violet spectrum. P1-c is characterized by a distinct dual-absorption peak at 404 nm (violet) and 591 nm (yellow), leading to a markedly black solution 19 . Subsequent adjustments to 0.7 equivalents of monomer 1 and 0.5 equivalents of monomer 3 result in a diminished absorption in the yellow spectrum and a strong peak at 431 nm. Advancing the proportion of monomer 1 to 0.9 equivalents and reducing monomer 3 to 0.1 equivalents eliminates the dual-band absorption, with P1-e exhibiting a novel peak at 447 nm, associated with the blue spectrum, and the solution turns yellow 26 . These findings underscore the ability to tailor the absorption properties of the polymer across different spectral regions by fine-tuning the ratios of monomers 1 and 3. Notably, a dual-band absorption and a darker appearance of the solutions are observed when the proportions of monomer 1 and compound 3 are within the range of 0.3-0.5 equivalents. The copolymerization of the above three monomers achieves dual-band absorption. We will thoroughly explore the impact of adding another monomer on the absorption effect. We hypothesized that increasing the proportion of monomer 4 would increase absorption in the key 400 nm to 550 nm region. As expected, P2-a exhibits a broad and intense absorption peak at 614 nm and the polymer solution exhibits dark hue, which is attributed to its overall high visible absorbance with minimal red-light transmission (Figure 1b). To our surprise, P2-b exhibits a broad absorption peak across the entire visible region. It shows comparable shifts in absorption and the 'merging' of both optical transitions as the length of ProDOT electron-rich block increases. This is due to reducing the concentration of electron-poor compounds along the conjugated backbone while increasing the length of the electron-rich segment results in a simultaneous bathochromic shift of the high-energy transition and a hypsochromic shift of the low-energy transition, leading to the 'merging' of the two transitions and no obvious peak window is observed 5 . To better present the absorption effect, we appropriately adjusted the concentration of the P2-b solution. Remarkably, P2-b exhibits broadly and highly absorbing across the entire visible spectrum (Figure 1c). It exhibits absorption that is both broader and more intense than what has been previously reported 4-6, 27-34 . This spectral behavior suggests that the material has been engineered to absorb light across the entire visible wavelength range, which is ideal for applications requiring efficient light harvesting, such as photovoltaic cells or light-sensitive sensors. Not surprisingly, P2-c exhibits dual peaks at 614 nm and 474 nm, belonging to red and blue light regions, respectively. P2-d shows a strong peak at 622 nm and a weaker peak at 451 nm, respectively. However, P2-e and P2-f both exhibit the lowest intensity of the short-wavelength absorption at around 460 nm due to its relatively low concentration of electron-rich moiety 6 . The broad absorption of P2 is primarily attributed to the formation of an extended conjugation through the polymerization of multiple functional monomers. The thermal stability of the P2a-f polymer series was evaluated by thermogravimetric analysis. Weight loss process is displayed in Figure S2. Table 1 shows the decomposition data of P2 polymers at 5%, 50% and a char yield at 800 °C in nitrogen atmosphere. Below 320 ℃, no significant weight loss was observed in these polymers. The onset degradation temperature of these polymers was range from 320 °C to 340 ℃. The temperature at 5% weight loss of P2-a, P2-b, P2-c, P2-d, P2-e, and P2-f is 332.01 ℃, 348.83 ℃, 326.27 ℃, 308.62 ℃, 300.62 ℃, 346.37 ℃. These polymers lose 50% of their weight at temperatures ranging from 397.28 o C to 413.62 o C. Besides, the residual carbonization of these polymers at 800 ℃ is 24-31wt %. Thermal analysis results showed that these polymers showed similar thermal stability due to their molecular skeleton. Most of them are relatively stable before 300 ℃ and begin to decompose at 340 ℃, which suggests that these polymers have stable good thermal stability. As shown in Table 1, the number average molecular weight of the polymers was about 10000 to 19000, and the polydispersity coefficient (PDI) was between 1.54 and 1.97, respectively. Conjugated polymers with larger molecular weights not only enhance the stability of the material, allowing it to maintain chemical stability for a long time, but also confer higher electrical conductivity, making the material more responsive to external electric fields. These polymers completely dissolved in most solvents such as CH 2 Cl 2 、CHCl 3 and DMF due to their polar long triethylene glycol (TEG) side chain improving the solubility 35-37 . Table 1. Thermal properties, molecular weight and HOMO and LUMO of the P2 polymer series Performance of ECDs As show in Figure2 a, ECDs are typically composed of two transparent conductive layers (substrate), EC layer, an ion-conductive layer and a counter electrode layer. The cyclic voltammogram (CV) and ECDs of the P1 are shown in Figure S3. The oxidation peak of P1-a is 0.80 V, and the reduction peak is 0.61 V. Photographs of the devices are shown in its neutral and color states. The device operates between 0.8 V and -0.1 V. The P1-a device displays blue in its neutral state and becomes transparent in coloring state. The oxidation peak of P1-b is 1.18 V, and the reduction peak appears at 0.95 V. P1-b is blue in its neutral state and similarly turns colorless in the bleached state. The oxidation peak of P1-c is 0.91 V, and the reduction peak is 0.70 V. The oxidation peak of P1-d is 0.76 V, and the reduction peak appears at 0.54 V. P1-c and P1-d manifest as deep black in their neutral state, but become semi-transparent at a voltage of -0.1 V. The oxidation peak of P1-e is 0.99 V, and the reduction peak appears at 0.72 V. P1-e appears yellow in neutral state and switches to green in the colored state. The oxidation voltage and reduction voltage of these devices are low. These copolymers undergo reversible electrochromic switch from a strongly neutral black to a highly transmissive oxidized state within a potential window of less than 1 V, representing an ideal parameter for low-driving-voltage device applications. The EC performance of the device in neutral state is consistent with its absorption spectrum in solution. When an applied voltage is present, the ECDs transition from a dark to a light color. Notably, the P1-c and P1-d ECDs exhibit dark in its neutral state and only partially absorbs in the visible spectrum. The spectroelectrochemical behavior of P2-b is displayed in Figure 2c. In the neutral state, P2-b shows strong absorption at wavelength around 681 nm. When P2-b is oxidized (increasing the applied voltage from 0 to 1.4 V), the device gradually becomes transparent due to the oxidation of the polymer, and the absorption peak strength of about 681 nm gradually decreases. When the oxidation voltage reaches 1.4 V, P2-b exhibits weaker absorption in the visible region, making it appear transparent. In the process of oxidation of the polymer, absorption diminishes in the visible spectrum, with a polaron transition in the near-infrared (800-1200 nm) and a weakening bipolaronic transition in the near-infrared. When fully oxidized, the resulting dual polarization absorption peak exceeds 1600 nm, allowing for effective reduction of visible light absorption with high transmittance 5, 6 . To measure the efficiency of ECDs in achieving optical modulation with a given voltage, coloration efficiency (CE) assessments were performed. Coloration efficiencies ( CE ) were evaluated by dividing the change in optical density (ΔOD) by the injected charge per unit area (Δ Q ) (eq 1): where ΔOD is defined as a log of the transmittance ratio of the bleached state ( T b ) to the colored state ( T c ). The variable ΔQ denotes the injected charge, which is determined by integrating the transient current profile. This integration process is detailed in Figure S4. As shown in Figure 2d, the coloration efficiency values were 762,1273, 887, 728, 548, and 229 cm²/C for P2-a, P2-b, P2-c, P2-d, and P2-e, respectively, which is favorably compared to the other ECP-based systems. The maximum coloration efficiency reached an impressive 1193 cm²/C, surpassing the previously reported ECDs coloration efficiencies (as compared to other work, see Table S1 ). High coloration efficiency, which means less charge is converted into greater optical density variation, is a desired parameter in ECDs. This performance is highly valuable in EC applications, as it means low energy consumption and high overall energy efficiency. To investigate the electrochemical behavior of P2 devices, cyclic voltammetry (CV) tests were conducted. As shown in Figure 3, the oxidation peaks of these device are between 0.5 V and 1 V and the reduction peaks of the devices are between 0.2 V ~ 0.5 V. The lower redox voltage not only increases the cyclic stability of the devices but also saves energy. In the process of oxidation, the color of all the devices switches from black-to-transmissive. We find that these devices exhibit reversible electrochromic transitions from an intensely opaque, neutral black state to a transparent oxidized state, all occurring within a potential window of less than 1 V, a desirable feature for low-voltage device applications. This enhancement is ascribed to the bipolar TEG side chains 35, 38 , whose synergistic effect enhances charge transport and increases ion diffusion rates, resulting in reduced driving voltages required for ECDs. Cyclic stability is one of the most crucial parameters for evaluating ECDs. However, degradation of their optical modulation is typically observed after several hundreds or thousands of cycles, and lifetime is also crucially dependent on the operational voltage range 39 .To investigate the cyclic stability and switching time of ECDs, we measured the transmittance change at a given wavelength. The switching time is defined as the time taken for the transmittance to reach 90% of its full change after the application of voltage. As depicted in Figure 4 (a), the optical contrast of P2-a is 30% and it maintains 99% even after switching for 2535718 s (126786 cycles). As shown in Figure 5(a), it requires 1.9 s of coloring and 1.9 s of bleaching. As shown in Figure 4 (b), the P1-b device remains extremely stable even after as many as 58735 s (2936 cycles). As presented in Figure 5(b), its coloring time is 0.95 s and the bleaching time is also 0.98 s. As shown in Figure 4(c), the P2-c device remained stable after 191713 s (9585 cycles) and the coloring time is 0.82 s and the bleaching time is 0.86 s (Figure5(c)). As shown in Figure 4(d), after 194812s (9740 cycles), the cyclic stability of P2-d fluctuates only slightly. Figure 5 (d) illustrates that the coloring time is 0.93 s and the bleaching time is 0.96 s. Figure 4 (e) shows the cyclic stability of the device after 101153 s (5075 cycles) and its coloring time is 0.93 s and a beaching time is 0.96 s (Figure 5e). As shown in Figure 4(f), the P2-f device, after 51411 s (2570 cycles), exhibits a slight decline in cyclic stability. Its coloring time is 3.75 s, and its bleaching time is 3.66 s. Fast switching time is attributed to the fact that copolymerization extends conjugation, thereby allowing π-electrons to travel more freely across the molecule 40 . This improves charge transport and enables a quicker response to electric fields, ultimately shortening the response times. In the quest for sustained long-term cyclic stability, it is imperative not only to constrain the low operational voltage range but also to meticulously uphold a dynamic equilibrium between electrons and ions at the active electrode interface during the redox process 41 . These devices exhibit outstanding cyclic stability and fast switching times, demonstrating that the P2 series polymers have excellent performance. This series of data fully demonstrates the high performance of these devices. To demonstrate the scalability of the device, a large-area ECD 100 cm² was fabricated, showcasing its potential for widespread application and facilitating its path towards industrialization (see Video 1). Generally, the darker the copolymer, the more difficult it is to switch to being transmissive. Its minimum transmittance is below 2%, and the contrast is about 30%, making it ideal materials for manufacturing smart automotive sunroofs (Figure 2b). To investigate further evaluate the colorimetric properties of different devices, we measured the color coordinates of each device in neutral and summarized the results as Table 2. P2-a demonstrates a notably dark hue with an L* value of 10.57, suggesting minimal lightness, and the color tends toward the red and blue regions, with a* and b* values of 10.53 and -14.93, respectively. This is consistent with the visible absorption spectrum of P2-a, as the polymer transmits a small amount of red light and slightly more blue light. P2-b, with an L* value of 19.17, is relatively darker yet exhibits nearly neutral a* and b* values, suggesting it's close to black. P2-c, with an L* value of 40.84, is one of the lighter shades and it looks mostly green and blue, because its a* and b* values are more on the negative side. P2-d is characterized by a medium lightness level with an L* value of 33.76 and exhibits green and blue tendencies with a* and b* values of -17.24 and -16.34, respectively. P2-e and P2-f, with L* values of 12.92 and 40.84, respectively, with greenish-blue chromaticity, aligning with their negative a* and b* values. They primarily appear black with slight hints of blue and green, which is consistent with their absorption curves showing lower absorption rates in the blue and green light regions. Table 2. L*a*b* values in neutral state of P2 ECDs P2-a P2-b P2-c P2-d P2-e P2-f L * 10.57 19.17 15.95 33.76 12.92 40.84 a * 10.53 0.78 -10.95 -17.2 -13.35 -17.44 b* -14.93 -0.35 -14.44 -16.34 -16.70 -29.71 Conclusion In this contribution, precise control of the absorption spectra of conjugated polymers was achieved by simply adjusting the feed ratios of four types of monomers in a random direct C–H arylation polymerization. We present the most broadly absorbing black-to-transmissive switching conjugated EC polymers, realized through the strategic selection of four functional monomers. A novel strategy has been implemented to enhance the performance of ECDs by synergistically improving the ionic conductivity of copolymers. The ECDs exhibit excellent overall performance, marked by high reversibility (≥ 126,786 cycles), superior coloration efficiency (≥ 1,273 cm 2 /C), and rapid switching times (0.82 s for coloring and 0.86 s for bleaching), suggesting that these copolymers possess exceptional properties. Performance comparisons with similar materials are detailed in Table 3 . This study not only highlights advancements in the design of high-performance black EC materials but also provides significant inspiration for other applications, such as organic photovoltaics and sensor technology. Table 3 Performance of ECDs compared to other similar work Number Color in the ox/red state Absorption range (nm) Voltage range (V/V) CE (cm 2 /C) Cyclic stability (cycles) 1 Black-to-transmissive 500–700 nm 350nm -450 nm -0.6 / 0.7 V - 10000 Ref 5 2 Green to transmissive 300–410 nm 450nm-620 nm -0.4 / 0.85 V - 10000 (loss 5%) Ref 42 2 Blue-to-transmissive 380–420 nm 500–740 nm -0.4 / 0.96 V - 10000 (loss 7%) Ref 43 4 Blue-to-transmissive 420–710 nm -1 / 1 V - Ref 11 5 Black-to-transmissive 400–700 nm − 0.6 / 1.5 V - 18000 (loss 8%) Ref 6 6 Black-to-transmissive 450–750 nm -0.6 / 1.6 V - 500 Ref 4 7 Black-to-transmissive 380–430 nm 450 − 760 nm -0.2 / 0.7 V - 360 Ref 29 8 Black-to-transmissive 450–600 nm -2 / 2 V - - Ref 28 9 Black-to-transmissive 400–700 nm -0.3 / 0.8 V 333 - Ref 31 10 11 12 Black-to-transmissive Black-to-transmissive Black-to-transmissive 400–470 nm 550–750 nm - - 1.6 / -1.6 V -0.6/ 0.8V -2.5/ 0V - - - 1000 4000 Ref 8 Ref 44 Ref 45 Black-to-transmissive 320–760 nm -0.1 /0.8 V 1273 126786 (loss 1%) This work Declarations Data availability The data used in this study are available from the corresponding author on reasonable request. Competing interests The authors declare no competing interests. Acknowledges This work is financially supported by Shenzhen Fundamental Research Program (No. GXWD20201231165807007-2020081011134000), Shenzhen Science and Technology Program (JSGG20220831094202004), NSFC (22275003). It also is supported by China Scholarship Council (No.202306290018, Recipient: Chen Dinghui). Author contributions H.M. and W.H. conceived the project. D.C. and Q.R. performed material synthesis, structural characterization, devices fabrication, and electrochromic measurements. D.C. also collaborated with T.Z. in synthesizing the material. Moreover, D.C., Q.R., and Z.T. designed the experiments. D.C. and H.M. wrote the manuscript with contributions from all authors during the review and editing process. Correspondence and requests for materials should be addressed to Hong Meng. References Gu CJ, A. B.Zhang, Y. M.Zhang, S. X. Emerging electrochromic materials and devices for future displays. 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Thieno[3,2-b]thiophene-based conjugated copolymers for solution-processable neutral black electrochromism. Polymer Chemistry 9 , 5608-5616 (2018). Liu J , et al. Enhancing Molecular n-Type Doping of Donor-Acceptor Copolymers by Tailoring Side Chains. Adv Mater 30 , 1704630-1704639 (2018). Meng B LJ, Wang L. Oligo(ethylene glycol) as side chains of conjugated polymers for optoelectronic applications. Polym Chem 11 , 1261-1270 (2020). Onorato JW , et al. Side chain engineering control of mixed conduction in oligoethylene glycol-substituted polythiophenes. Journal of Materials Chemistry A 9 , 21410-21423 (2021). Liu J , et al. Amphipathic Side Chain of a Conjugated Polymer Optimizes Dopant Location toward Efficient N-Type Organic Thermoelectrics. Adv Mater 33 , e2006694 (2021). Wen RT, Granqvist CG, Niklasson GA. Eliminating degradation and uncovering ion-trapping dynamics in electrochromic WO 3 thin films. Nat Mater 14 , 996-1001 (2015). Mikie T , et al. Extended π-Electron Delocalization in Quinoid-Based Conjugated Polymers Boosts Intrachain Charge Carrier Transport. Chemistry of Materials 33 , 8183-8193 (2021). Ye LL, X. A dynamic stability design strategy for lithium metal solid state batteries. Nature 593 , 218-222 (2021). Beaujuge PM, Ellinger S, Reynolds JR. Spray processable green to highly transmissive electrochromics via chemically polymerizable donor-acceptor heterocyclic pentamers. Adv Mater 20 , 2772–2776 (2008). Amb CM, Beaujuge PM, Reynolds JR. Spray-processable blue-to-highly transmissive switching polymer electrochromes via the donor-acceptor approach. Adv Mater 22 , 724–728 (2010). Hernandez TS, Barile CJ, Strand MT, Dayrit TE, Slotcavage DJ, McGehee MD. Bistable black electrochromic windows based on the reversible metal electrodeposition of Bi and Cu. ACS Energy Letters 3 , 104-111 (2017). Islam SM, Hernandez TS, McGehee MD, Barile CJ. Hybrid dynamic windows using reversible metal electrodeposition and ion insertion. Nat Energy 4 , 223-229 (2019). Pouliot JR, Grenier F, Blaskovits JT, Beaupre S, Leclerc M. Direct (hetero)arylation polymerization: Simplicity for conjugated polymer synthesis. Chem Rev 116 , 14225-14274 (2016). Methods Synthesis and characterization The detailed synthetic procedures for compounds are provided in the Supporting Information (SI). Polymer1 series (P1) and polymer2 series (P2) was synthesized according to Figure1. In this work, we synthesize polymers through direct C–H arylation polymerization (DArP). DArP is an environment friendly polymerization for the donor–acceptor (D–A) type 46 . The molecular weights of polymers are provided in Table 1. Materials Tri(ethylene glycol) monoethyl ether, ethyl 2-hydroxybenzoate, 2,2-bis(bromomethyl)-1,3-propanediol, Potassium carbonate (K 2 CO 3 ), chloroform, Pd(OAC) 2 , PiVOH, tri(ethylene glycol) monoethyl ether were purchased from Bide. Tetrahydrofuran (THF), ethanol, methanol, N,N-dimethylformamide (DMF), N,N-dimethylacetamide (DMAc) were bought from Aladdin. 2-dibromo-9-fluorenone, 4-toluene sulfonyl chloride, methanesulfonic acid purchased from Energy-chemical. Indium tin oxide (ITO) glasses were purchased from south China Xiangcheng Technology Co., LTD. Measurements The 1H NMR and 13C NMR spectra were recorded in CDCl 3 solution at room temperature using Bruker AVANCE 500 (or 400) NMR spectrometers. Absorption spectra were obtained using a PerkinElmer Lambda 750 spectrophotometer. Cyclic Voltammetry (CV) curves were generated using a Gamry 1000B electrochemical workstation. For potential-dependent in-situ absorption measurements, the Gamry 1000B workstation was used in conjunction with the PerkinElmer Lambda 750 spectrophotometer. Thermal gravimetric analysis (TGA) was performed under a nitrogen (N 2 ) atmosphere from 30 to 800 °C at a heating rate of 10 °C/min using a Mettler Toledo TGA2 instrument. Average molecular weights and polydispersity indices (PDIs) were determined using gel permeation chromatography (Waters ACQUITY Advanced Polymer Chromatograph). L*a*b* values were based on the International Commission's 1931 L*a*b* color model. Fabrication of devices The working electrode was prepared by bar coating method, and 40 mg/mL polymer solution was coated on indium tin oxide (ITO) substrate with a size of 3 × 3 cm. The counter electrode was prepared by bar coating 15 mg/mL PB solutionon the ITO substrate. Before device fabrication, ITO coated with polymer or PB was vacuum-dried at 60 °C for half an hour. The solid-state electrolyte was uniformly dispersed on the surface of the polymer film. Subsequently, ITO coated with PB was pressed onto working electrode. The device is then cured using ultraviolet light for 10 seconds to bond the working electrode and the counter electrode together. Subsequently, the device was encapsulated using UV and thermosetting OLED adhesive. Finally, it was cured with ultraviolet light for 20 seconds, followed by vacuum drying at 80 ℃ for 50 minutes. Additional Declarations There is NO Competing Interest. Supplementary Files SupplementaryInformation.pdf video.mp4 Video Cite Share Download PDF Status: Published Journal Publication published 30 Sep, 2024 Read the published version in Nature Communications → Version 1 posted You are reading this latest preprint version Research Square lets you share your work early, gain feedback from the community, and start making changes to your manuscript prior to peer review in a journal. As a division of Research Square Company, we’re committed to making research communication faster, fairer, and more useful. We do this by developing innovative software and high quality services for the global research community. Our growing team is made up of researchers and industry professionals working together to solve the most critical problems facing scientific publishing. Also discoverable on Platform About Our Team In Review Editorial Policies Advisory Board Help Center Resources Author Services Accessibility API Access RSS feed Manage Cookie Preferences © Research Square 2026 | ISSN 2693-5015 (online) Privacy Policy Terms of Service Do Not Sell My Personal Information {"props":{"pageProps":{"initialData":{"identity":"rs-3939829","acceptedTermsAndConditions":true,"allowDirectSubmit":false,"archivedVersions":[],"articleType":"Article","associatedPublications":[],"authors":[{"id":274250312,"identity":"25050a4a-77ca-45fd-aa35-2877a17be271","order_by":0,"name":"Dinghui Chen","email":"","orcid":"","institution":"Frontiers Science Center for Flexible Electronics (FSCFE) \u0026 Shaanxi Institute of Flexible Electronics (SIFE), Northwestern Polytechnical University (NPU), 127 West Youyi Road, Xi'an 710072, China","correspondingAuthor":false,"prefix":"","firstName":"Dinghui","middleName":"","lastName":"Chen","suffix":""},{"id":274250313,"identity":"3d693da5-a3ef-473d-b5a3-6f48b9d4cac2","order_by":1,"name":"Zizheng Tong","email":"","orcid":"","institution":"School of Advanced Materials, Peking University Shenzhen Graduate School, Peking University, Shenzhen, 518055, China","correspondingAuthor":false,"prefix":"","firstName":"Zizheng","middleName":"","lastName":"Tong","suffix":""},{"id":274250314,"identity":"5410ea9f-eff3-406f-87c5-0007de437d9b","order_by":2,"name":"Qiushi Rao","email":"","orcid":"","institution":"School of Advanced Materials, Peking University Shenzhen Graduate School, Peking University, Shenzhen, 518055, China","correspondingAuthor":false,"prefix":"","firstName":"Qiushi","middleName":"","lastName":"Rao","suffix":""},{"id":274250311,"identity":"d17e9a8a-5b72-4597-b955-ae50a19bcb86","order_by":3,"name":"Hong Meng","email":"data:image/png;base64,iVBORw0KGgoAAAANSUhEUgAAAZAAAAAyAQMAAABI0h/eAAAABlBMVEX///8AAABVwtN+AAAACXBIWXMAAA7EAAAOxAGVKw4bAAAA2ElEQVRIiWNgGAWjYJACZhDBz8AGZxOpRbKBZC0GB4jVotvee/h1QcUdu82329IkGCqsExvYzx7Aq8XszLk06xlnniVvu3PsmATDmfTEBp68BPxabuSYGfO2HU42u5HeJsHYdjixQYLHAL+W+28gWoxngLT8I0bLDR7jx0AtdgYSacckGBuI0XImx4yZ58zhBIk7x5ItEo6lG7fx5BDQcvyM8WeeisP2/LPbDG98qLGW7Wc/g18LELBJAAmge4BkAohLSD0QMH8AEvYMEkQoHQWjYBSMgpEJACFRRjvXL/vvAAAAAElFTkSuQmCC","orcid":"https://orcid.org/0000-0001-5877-359X","institution":"School of Advanced Materials, Peking University Shenzhen Graduate School, Peking University, Shenzhen, 518055, China","correspondingAuthor":true,"prefix":"","firstName":"Hong","middleName":"","lastName":"Meng","suffix":""},{"id":274250315,"identity":"17661a88-9ca3-44cd-b937-d569ef2a39a0","order_by":4,"name":"Wei Huang","email":"","orcid":"https://orcid.org/0000-0001-7004-6408","institution":"Frontiers Science Center for Flexible Electronics (FSCFE) \u0026 Shaanxi Institute of Flexible Electronics (SIFE), Northwestern Polytechnical University (NPU), 127 West Youyi Road, Xi'an 710072, China","correspondingAuthor":false,"prefix":"","firstName":"Wei","middleName":"","lastName":"Huang","suffix":""}],"badges":[],"createdAt":"2024-02-08 11:53:09","currentVersionCode":1,"declarations":"","doi":"10.21203/rs.3.rs-3939829/v1","doiUrl":"https://doi.org/10.21203/rs.3.rs-3939829/v1","draftVersion":[],"editorialEvents":[{"content":"https://doi.org/10.1038/s41467-024-52430-2","type":"published","date":"2024-09-30T04:00:00+00:00"}],"editorialNote":"","failedWorkflow":false,"files":[{"id":51527985,"identity":"a2fa88f0-083f-4252-a526-0dfbaa4323ea","added_by":"auto","created_at":"2024-02-23 06:22:55","extension":"png","order_by":1,"title":"Figure 1","display":"","copyAsset":false,"role":"figure","size":162540,"visible":true,"origin":"","legend":"\u003cp\u003e(a) Normalized UV-Vis solution absorption spectra of P1 polymers in chloroform solution (0.2 mg/mL); (b) Normalized UV-Vis solution absorption spectra of P2 polymers in chloroform solution (0.2 mg/mL); (c) Normalized UV-Vis solution absorption of Polymer P2-b in chloroform (0.25 mg/mL); (d) Energy level diagram of the P2 polymers;(e) P2 Coloration efficiencies efficiency.\u003c/p\u003e","description":"","filename":"1.png","url":"https://assets-eu.researchsquare.com/files/rs-3939829/v1/779f315667b38dbc0caf2b96.png"},{"id":51527986,"identity":"b0510b87-873e-4655-b007-4ec4fdb71182","added_by":"auto","created_at":"2024-02-23 06:22:55","extension":"png","order_by":2,"title":"Figure 2","display":"","copyAsset":false,"role":"figure","size":216220,"visible":true,"origin":"","legend":"\u003cp\u003e(a)The structure of EDCs; (b) Smart automotive sunroof; (c) Spectroelectrochemistry of P2-b devices at different voltage; (d) Energy level diagram of the P2 polymers; (d) P2 Coloration efficiencies efficiency.\u003c/p\u003e","description":"","filename":"2.png","url":"https://assets-eu.researchsquare.com/files/rs-3939829/v1/892659a972a742c273cf6c23.png"},{"id":51528449,"identity":"c8874d5e-1ea4-4f5c-91e8-38303c8b79f8","added_by":"auto","created_at":"2024-02-23 06:30:56","extension":"png","order_by":3,"title":"Figure 3","display":"","copyAsset":false,"role":"figure","size":123158,"visible":true,"origin":"","legend":"\u003cp\u003e(a), (b), (c), (d), (e) and (f) is CV curves of P2-a, P2-b, P2-c, P2-d, P2-e and P2-f.\u003c/p\u003e","description":"","filename":"3.png","url":"https://assets-eu.researchsquare.com/files/rs-3939829/v1/92909ac087c776b585ccecb3.png"},{"id":51527990,"identity":"170840ba-09d4-4d2d-abc8-bfb67c09e7f2","added_by":"auto","created_at":"2024-02-23 06:22:56","extension":"png","order_by":4,"title":"Figure 4","display":"","copyAsset":false,"role":"figure","size":60103,"visible":true,"origin":"","legend":"\u003cp\u003e\u0026nbsp;(a), (b), (c), (d), (e) and (f) is transmittance changes of P2-a, P2-b, P2-c, P2-d, P2-e and P2-f. Transmittance changes with pulse width from 10 s of devices with applied potential between -0.1 and 0.8V, respectively.\u003c/p\u003e","description":"","filename":"4.png","url":"https://assets-eu.researchsquare.com/files/rs-3939829/v1/2dd14c19e454c42c7de9599d.png"},{"id":51527989,"identity":"c5e1c1a7-8901-48f6-a6e6-3af44717fc62","added_by":"auto","created_at":"2024-02-23 06:22:56","extension":"png","order_by":5,"title":"Figure 5","display":"","copyAsset":false,"role":"figure","size":120796,"visible":true,"origin":"","legend":"\u003cp\u003e(a), (b), (c), (d), (e) and (f) are switch time of P2–a, P2−b, P2-c, P2−d a, P2-e and P2-f.\u003c/p\u003e","description":"","filename":"5.png","url":"https://assets-eu.researchsquare.com/files/rs-3939829/v1/02a275a260a23a877a2ba2f4.png"},{"id":65670275,"identity":"f6c463c3-6e6b-47d6-b9c3-c1d4a052dcab","added_by":"auto","created_at":"2024-10-01 07:05:57","extension":"pdf","order_by":0,"title":"","display":"","copyAsset":false,"role":"manuscript-pdf","size":1338956,"visible":true,"origin":"","legend":"","description":"","filename":"manuscript.pdf","url":"https://assets-eu.researchsquare.com/files/rs-3939829/v1/ae12ce23-abc0-484e-b587-5b66899c4762.pdf"},{"id":51527987,"identity":"cc21c12e-f910-42be-bfeb-277163889363","added_by":"auto","created_at":"2024-02-23 06:22:55","extension":"pdf","order_by":1,"title":"","display":"","copyAsset":false,"role":"supplement","size":1412398,"visible":true,"origin":"","legend":"\u003cp\u003e\u003cbr\u003e\u003c/p\u003e","description":"","filename":"SupplementaryInformation.pdf","url":"https://assets-eu.researchsquare.com/files/rs-3939829/v1/6b0667aa112d4466af383d83.pdf"},{"id":51527992,"identity":"05ae6c12-0246-44c6-bcd0-e07c6fcd11a9","added_by":"auto","created_at":"2024-02-23 06:22:56","extension":"mp4","order_by":2,"title":"","display":"","copyAsset":false,"role":"supplement","size":2793515,"visible":true,"origin":"","legend":"\u003cp\u003eVideo\u003c/p\u003e","description":"","filename":"video.mp4","url":"https://assets-eu.researchsquare.com/files/rs-3939829/v1/c04fe791889c06e1fab63244.mp4"}],"financialInterests":"There is \u003cb\u003eNO\u003c/b\u003e Competing Interest.","formattedTitle":"Unlocking the Full Spectrum: A Paradigm Shift in Electrochromic Devices with High-Performance Black Conjugated Polymers","fulltext":[{"header":"Introduction","content":"\u003cp\u003eRecently, the development of advanced EC materials has become a cornerstone that intertwines function with environmental sustainability. The core of this advancement is the design of EC materials, which have revolutionized the field due to their ability to undergo reversible optical transitions in response to electrical stimulus\u003csup\u003e1, 2\u003c/sup\u003e. These materials play an important role in the emerging field of smart technologies, such as energy-efficient displays, smart windows, and smart sunroof \u003csup\u003e3\u003c/sup\u003e, which are changing our lives. However, the widespread practical deployment of EC materials faces several significant obstacles, such as limited stability, slow switching times, and low coloration efficiency. To unlock its full potential, it is imperative to design EC copolymers with high performance that address these challenges.\u003c/p\u003e \u003cp\u003eBlack-to-transmissive EC materials are particularly eye-catching among EC materials. Black materials have the ability to absorb light almost completely, offering the possibility of improving energy efficiency in buildings and vehicles. However, the development of black ECDs still remains challenging task due to the complexity of broad absorbing spectrum modulation to cover the whole visible region homogeneously\u003csup\u003e4\u003c/sup\u003e. In their seminal work, Reynolds et al. developed copolymers using 2,1,3-benzothiadiazole (BTD) and 3,4-bis(2-ethylhexyloxy)thiophene (DOT-(OEtHx)\u003csub\u003e2\u003c/sub\u003e), revealing limited absorption in the 420\u0026ndash;550 nm range \u003csup\u003e5\u003c/sup\u003e(\u003cb\u003eFigure \u003cspan refid=\"MOESM1\" class=\"InternalRef\"\u003eS1\u003c/span\u003ea)\u003c/b\u003e. In their later work, they innovatively synthesized electrochromic polymers capable of transitioning from black to transmissive using a Stille polymerization approach with distannyl and distannyl 3,4-propylenedioxythiophene (ProDOT-(CH2OEtHx)\u003csub\u003e2\u003c/sub\u003e), along with 2,4,7-dibromo-2,1,3-benzothiadiazole. While the absorption range improved, challenges persisted with insufficient intensity in the 360\u0026ndash;480 nm range \u003cb\u003e(Figure \u003cspan refid=\"MOESM1\" class=\"InternalRef\"\u003eS1\u003c/span\u003eb\u003c/b\u003e)\u003csup\u003e6\u003c/sup\u003e. In parallel, Bao et al. utilized poly(3-hexylthiophene-2,5-diyl) (P3HT) in stretchable electronic skin, noting that the P3HT ECDs demonstrated relatively weak absorption in the 400\u0026ndash;500 nm range under various stress conditions ( \u003cb\u003eFigure \u003cspan refid=\"MOESM1\" class=\"InternalRef\"\u003eS1\u003c/span\u003ec\u003c/b\u003e)\u003csup\u003e7\u003c/sup\u003e. Leveraging direct C\u0026ndash;H arylation and Stille polymerization for synthesizing black materials garnered significant interest. Recently, a novel black polymer was synthesized using 3,3-bis((2-ethylhexyloxy)methyl)-3,4-dihydro-2H-thieno[3,4-b][\u003cspan citationid=\"CR1\" class=\"CitationRef\"\u003e1\u003c/span\u003e, \u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e4\u003c/span\u003e]dioxepine and 4,7-dibromo-2,1,3-benzothiadiazole monomers through a concerted metalation-deprotonation pathway \u003csup\u003e4\u003c/sup\u003e. Although its absorption in the 400\u0026ndash;500 nm range remained suboptimal (\u003cb\u003eFigure \u003cspan refid=\"MOESM1\" class=\"InternalRef\"\u003eS1\u003c/span\u003ed\u003c/b\u003e). Yan et al. explored this by integrating diverse spacing units such as carbazole, naphthalene, and phenylene into a ProDOT and BTD copolymer, yet observed a persistent weak absorption in the 400\u0026ndash;500 nm spectrum (\u003cb\u003eFigure \u003cspan refid=\"MOESM1\" class=\"InternalRef\"\u003eS1\u003c/span\u003ee\u003c/b\u003e)\u003csup\u003e8\u003c/sup\u003e. However, there is still a weak absorption of varying degrees in the 400\u0026ndash;500 nm (Figure \u003cspan refid=\"MOESM1\" class=\"InternalRef\"\u003eS1\u003c/span\u003ee). Although alternative methods have been explored to develop black materials that can absorb all visible light, these attempts have not yet met the expected outcomes\u003csup\u003e5, 6, 9\u0026ndash;19\u003c/sup\u003e. Up to now, synthesizing true black conjugated polymers remains a challenging frontier, as it demands precise control of the molecular structure, and requires a balance between broad-spectrum absorption, stability, and processability\u003csup\u003e6\u003c/sup\u003e.\u003c/p\u003e \u003cp\u003eIn the EC field, simultaneously achieving ultra-high stability, fast switching times, and high coloration efficiency in black EC conjugated polymers is a significant challenge \u003csup\u003e20\u0026ndash;22\u003c/sup\u003e. Most materials only exhibit high performance in one or two parameters, and it is very rare to meet three parameters simultaneously\u003csup\u003e23\u0026ndash;25\u003c/sup\u003e. This difficulty is primarily attributable to three major challenges. Firstly, conjugated polymers inherently exhibit low ionic conductivity. This limitation hinders the effective movement of ions, leading to a decrease in the overall performance of devices that incorporate these polymers. Secondly, the complexity of molecular design necessitates precise control over the structure, including monomer selection, polymerization methods, and chain arrangement, where enhancing one property may adversely affect others. Thirdly, the optimization of ECD properties involves inherent trade-offs: enhancing stability often necessitates more rigid molecular architectures, which can prolong the switching times; concurrently, improved coloration efficiency may demand more complex molecular structures, potentially compromising stability and increasing switching times.\u003c/p\u003e \u003cp\u003eTo address the above challenges, in this work, we strategically selected four types of monomers to design and synthesize high-performance EC materials. To address the limited absorption range of conjugated polymers in the visible spectrum, we introduced fluorene derivatives as additional monomers and simultaneously replaced the alkyl side chains of ProDOT with triethylene glycol (TEG) side chains to enhance the absorption properties of the copolymers. By adjusting the ratios of the four monomers, black copolymers were successfully synthesized. To tackle the challenges of limited stability, slow switching times, and low coloration efficiency in ECDs, we enhanced electronic conductivity by extending the conjugation lengths of four monomers, and introduced ester and TEG side chains into the copolymer to boost its ionic conductivity through the synergistic effect, thereby comprehensively improving the performance of ECDs. The bar-coating polymer thin film exhibited a deep black neutral state and attained transmissive state upon full oxidation. This work offers a novel strategy for designing high-performance black EC materials, laying the \u003c/p\u003e"},{"header":"Results and discussion","content":"\u003cp\u003e\u003cstrong\u003eProperties of polymers\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eFigure1.\u0026nbsp;(a) Normalized UV-Vis solution absorption spectra of P1 polymers in chloroform solution (0.2 mg/mL); (b) Normalized UV-Vis solution absorption spectra of P2 polymers in chloroform solution (0.2 mg/mL);\u0026nbsp;(c) Normalized UV-Vis solution absorption of Polymer P2-b in chloroform (0.25 mg/mL); (d) Energy level diagram of the P2 polymers;(e) P2 Coloration efficiencies efficiency.\u003cbr\u003e\u0026nbsp; \u0026nbsp;In the P1a-e polymer series, the concentration of monomer 1 was incrementally increased from 10 mol% to 90 mol%, while that of monomer 3 was correspondingly reduced from 90 mol% to 10 mol%. Figure 1(a) illustrates that the UV-Vis spectrum of P1-a features a pronounced absorption peak at 594 nm, accompanied by a less intense peak at 324 nm, resulting in a blue-colored solution. The spectrum of P1-b reveals a broad absorption peak at 596 nm and an additional peak at 366 nm. Moreover, upon adjusting the proportion of monomer 1 to 0.5 equivalents and reducing monomer 3 to 0.5 equivalents, a prominent new peak emerges at 404 nm, indicative of the violet spectrum. P1-c is characterized by a distinct dual-absorption peak at 404 nm (violet) and 591 nm (yellow), leading to a markedly black solution\u003csup\u003e19\u003c/sup\u003e. Subsequent adjustments to 0.7 equivalents of monomer 1 and 0.5 equivalents of monomer 3 result in a diminished absorption in the yellow spectrum and a strong peak at 431 nm. Advancing the proportion of monomer 1 to 0.9 equivalents and reducing monomer 3 to 0.1 equivalents eliminates the dual-band absorption, with P1-e exhibiting a novel peak at 447 nm, associated with the blue spectrum, and the solution turns yellow\u003csup\u003e26\u003c/sup\u003e. These findings underscore the ability to tailor the absorption properties of the polymer across different spectral regions by fine-tuning the ratios of monomers 1 and 3. Notably, a dual-band absorption and a darker appearance of the solutions are observed when the proportions of monomer 1 and compound 3 are within the range of 0.3-0.5 equivalents.\u003c/p\u003e\n\u003cp\u003eThe copolymerization of the above three monomers achieves dual-band absorption. We will thoroughly explore the impact of adding another monomer on the absorption effect. We hypothesized that increasing the proportion of monomer 4 would increase absorption in the key 400 nm to 550 nm region. As expected, P2-a exhibits a broad and intense absorption peak at 614 nm and the polymer solution exhibits dark hue, which is attributed to its overall high visible absorbance with minimal red-light transmission (Figure 1b). To our surprise, P2-b exhibits a broad absorption peak across the entire visible region. It shows comparable shifts in absorption and the \u0026apos;merging\u0026apos; of both optical transitions as the length of ProDOT electron-rich block increases. This is due to reducing the concentration of electron-poor compounds along the conjugated backbone while increasing the length of the electron-rich segment results in a simultaneous bathochromic shift of the high-energy transition and a hypsochromic shift of the low-energy transition, leading to the \u0026apos;merging\u0026apos; of the two transitions and no obvious peak window is observed\u003csup\u003e5\u003c/sup\u003e.\u0026nbsp;To better present the absorption effect, we appropriately adjusted the concentration of the P2-b solution. Remarkably, P2-b exhibits broadly and highly absorbing across the entire visible spectrum (Figure 1c).\u0026nbsp;It exhibits absorption that is both broader and more intense than what has been previously reported\u0026nbsp;\u003csup\u003e4-6, 27-34\u003c/sup\u003e. This spectral behavior suggests that the material has been engineered to absorb light across the entire visible wavelength range,\u0026nbsp;which is ideal for applications requiring efficient light harvesting, such as photovoltaic cells or light-sensitive sensors.\u0026nbsp;Not surprisingly, P2-c exhibits dual peaks at 614 nm and 474 nm, belonging to red and blue light regions, respectively.\u0026nbsp;P2-d shows a strong peak at 622 nm and a weaker peak at 451 nm, respectively. However, P2-e and P2-f both exhibit the lowest intensity of the short-wavelength absorption at around 460 nm due to its relatively low concentration of electron-rich moiety\u003csup\u003e6\u003c/sup\u003e. The broad absorption of P2 is primarily attributed to the formation of an extended conjugation through the polymerization of multiple functional monomers.\u003c/p\u003e\n\u003cp\u003eThe thermal stability of the P2a-f polymer series was evaluated by thermogravimetric analysis. Weight loss process is displayed in Figure S2. Table 1 shows the decomposition data of P2 polymers at 5%, 50% and a char yield at 800 \u0026deg;C in nitrogen atmosphere. Below 320 ℃, no significant weight loss was observed in these polymers. The onset degradation temperature of these polymers was range from 320 \u0026deg;C to 340 ℃. The temperature at 5% weight loss of P2-a, P2-b, P2-c, P2-d, P2-e, and P2-f is 332.01 ℃, 348.83 ℃, 326.27 ℃, 308.62 ℃, 300.62 ℃, 346.37 ℃. These polymers lose 50% of their weight at temperatures ranging from 397.28 \u003csup\u003eo\u003c/sup\u003eC to 413.62 \u003csup\u003eo\u003c/sup\u003eC. Besides, the residual carbonization of these polymers at 800 ℃ is 24-31wt %. Thermal analysis results showed that these polymers showed similar thermal stability due to their molecular skeleton. Most of them are relatively stable before 300 ℃ and begin to decompose at 340 ℃, which suggests that these polymers have stable good thermal stability.\u003c/p\u003e\n\u003cp\u003eAs shown in Table 1, the number average molecular weight of the polymers was about 10000 to 19000, and the polydispersity coefficient (PDI) was between 1.54 and 1.97, respectively. Conjugated polymers with larger molecular weights not only enhance the stability of the material, allowing it to maintain chemical stability for a long time, but also confer higher electrical conductivity, making the material more responsive to external electric fields. These polymers completely dissolved in most solvents such as CH\u003csub\u003e2\u003c/sub\u003eCl\u003csub\u003e2\u003c/sub\u003e、CHCl\u003csub\u003e3\u003c/sub\u003e and DMF due to their polar long triethylene glycol (TEG) side chain improving the solubility\u003csup\u003e35-37\u003c/sup\u003e.\u0026nbsp;\u003c/p\u003e\n\u003cp\u003e\u003cimg 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\"\u003e\u003cbr\u003e\u003c/p\u003e\n\u003cp\u003eTable 1. Thermal properties, molecular weight and HOMO and LUMO of the P2 polymer series\u003c/p\u003e\n\u003cp\u003e\u003cimg 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iCOO6DPJBg864gGg4f9zxaBBg/rkA3cUj+J6RQLKSh0wYIB/QNDChQu77V+viIiISDXwxFUeCnjyySd3XDXiioP0PMV+U/Z0WnvYjOkryYY9gGmrrbbaJOHmwUsk5Vwljv9dTG+leDSmVySgPHGTf7zNE6bCx3yLiIhI6+Nffpxyyim+ueOvfvWrZGg7nvppFTqu0pEsSfdR7DfFMrPs8b9fQZhs9OYWefa/W8MnAMd+8pOfuP/+3/97Rzy+/e1vd7RYpLyQtIX/XcLKD1eXJ0+e3DGc91bOwHgM57tMI2bT5ff4Xr3pdYdG44G0mJg4NvZZOPyHP/xhJWNRCDeCioiIiFTRunXr2moV/dQnroYPc6FLG0e6rqqx5wFIzFuz2MNmeAhRGuLAZ731yacsH+ub9R4/RInPeJr9yJEjfYzCh++wzg4//PBNhjGuDeP1a1/7WtvChQt9v/1WHGtiS9mMy0E8ftHpbY6uxgPx8ofS4gX62QZMlWJRlBJQERERqSSrnKVVrmCfU/HT03C7V1VjT2X+n/7pn5K+8rGcVNizkg0q+Xlxa3W27EU6kpuwXBAbnggbDiN5sgSIeBG3OHFPS7Cuv/761OSM4fvvv78fXm963WFz4oG0mJisz5577rlOy12VWDSi1z0FV0RERHoH+wf+b731VmqzNvu8Volyb7/9tm+mZs3VwveGJmvW9Iz3YRO4BQsW+KZq4fh9WdHY1+qS7tZbb/XNCvlPBNtuu62PpzXtsyaADKc5r41D/EHc7Tth7MNp2XC+w0N+ahXrpjT35Te5v5OHMYH7Ypk/6/hs2LBh7uWXX+7UFJPl3meffTqN24z57w533313xxN863W///3vO5qbgvtmiUM4jAf3HHfccf79xRdf7ONmD7nKQpnacsstfRdavny5H8Z9uDwQquj0NsfmxANpMTF89oMf/GCTz2hGy/KhSrFohBJQERERaVlUwM477zz3hz/8wVfUVq1a5a666ir/Ge8feOABPw5JwP/9v//X/8sMhr/xxhv+/T//8z/7f53Bw2RmzJjR0v8Wo5mIG8nkCy+84OP6X//1X+7ZZ5/1SdhDDz3k7yGl4oylS5f6dcF9c7yno4JusSfhJIl75513/Lpat26dH3711Vf7Ewb0N6MizW/GSUVWR2ICyt6UKVPc/PnzfVy+//3v+xMmVUkEysLJCO6bjZN2HtzDfbTEifeWjIZIUsOEnnJEov/f/tt/63gYFts3/wbn888/9wkdsa43vWYjJpzEiZ+aCz77z//8z03uMSZOnOiwpLRVY6EEVERERFqWJTgkkSeccIIftssuu3S8N3vvvbdPRkmKqLDxBFPwfZKD008/3Q+XxlHhXbFihU/mudqSdpWHZIOng/KwSLvqQz9XZh577LFkzPZpkWBeeOGF/ioOJwVOOukk/9nKlSv9v36xRKQVkGTzrzlYVpKF9957r+7/Ce2NWHbiQDJkSTqJuCWWxOlv/uZvNolNWmLKtOwKIEjWOFFB2bKErpHpNQvLgXBZDJ+RaMZlPV72Vo2FElARERHp9ahs0RSUM/4kOCSphkoxSIykccRtwoQJHZVlksgXX3zRV3jtyhcnCEaNGuXXw5NPPtlxgoATA1zl4eopmBZNbA8++GB/BYj1xThM5xe/+EUlEodGMO+77babT5xHjx7t/umf/skP62vspEN4coJ1W299coLiq1/9qjvkkEN8P+XHrgDuueeevozcdtttbty4cbkJnYmn10xpMTF8Fv+fXbYBltHKTyvHQgmoiIiI9Hr333+/v9piTSMNydKjjz7qr65xxYB+aZw1k6XiS5NT7gGlokw/V74YBruK+b//9//2VzmpRJOo0gyXCjauu+46X5mmmSr/1oR1wnTWr1/fkdS2kqFDh/qrUh9//HGf/HeBrK+4qSnrkzJjTUxJlHbccUd37733+vHpaJLNFTqurFuSxvfCpIpWDSRQnPwIE7qi02sWliM8EQPue7Z7g7klgJgxHph//o3L//gf/8P3o6Vj0SYiIiLSojZs2PgvEPj3AvaepzvylFLe86TKWgLg/w0C/dbxtFK68HOeCFmrGCdTlyLCdRD+mwewDsKnxRJrnpq7fPlyH2u+Q9xZXyD2rBNbP2+++aYfzuf0L1iwwPe3CouNzTv9fQnrzbY34sDypw0D69rWPWWCpx3bZxZHPrNtlOnQ8d7KEp2Vt7zpNVO4/GEX73v4Vyu2z+I1/vcp4XdaLRb9+FObGRERERER6Ua33367b57MlV6ubj399NPujjvu2OTePpG+RE1wRURERES6GU2HSThBM8gzzjjD7bHHHr5fpC9TAioiIiIi0s1IOvk/jDwohqcAcw8k9/zp6qf0dWqCKyIiIiIiIqXQFVAREREREREphRJQERERERERKYUSUBERERERESmFElAREREREREphRJQERERERERKYUSUBERERERESmFElAREREREREphRJQERERERERKYUSUBERERERESmFElAREREREREphRJQERERERERKUWvSkDffvttN3PmTLf11lsnQ0SkCkaOHOm3zaKef/55d9ZZZ7nDDz88GbKpTz75xM2fP98NGTLEjx/j87zvi4iIiEj5Sk9ASRKpWJIk9uvXz1cer7nmGl9ZZPjmmDFjhrvyyivdZ599lgwRKubEuV6XVoHv7RSbxrCdxrFhmEmLZ1cdddRR7pZbbkn60t1+++3uxz/+sXvrrbeSIRu99tpr7pvf/KY799xzkyE9gwTXlrXIiS8ScRtfyXE+xVZERKR3KjUBXbRokRs8eLD79NNP3TPPPOPa2trcn/70J7fTTju5XXfdtW6Fsx6mTxIqG61du9ZNnTrVffzxxz7eK1as8MN5pZ/hEyZM8OP1NYpNY6ZPn+5jM2LECN+/ZMkSP8wceOCBHTGcN2+ej6F5+eWX3ezZs5O++thH1MNv33vvvUnfRpzMOuaYY9zDDz/sxo0blwztGU8++aR79dVX/XtOfLEPykKC/sorr/j3fIfvSjbFVkREpHcqLQGlgjBp0iRfoacisddee/nh22yzjZs4caJPSLvDVlttlbwTvPvuu27atGk+zmkYzlUkxutrFJvGkWQ+8MADbsCAAe4nP/lJMnSjm266yS1cuNBNmTIlGdKzttxyy+TdRlwZHTNmTMc+pqfxOyTlxOSSSy5Jhm6K2IwdO9a/L2veWp1iKyIi0vuUloDOmjXLv9JENg2VBq5GSffiKtEuu+yS9KUj9uGVrL5CsekaYnbxxRf7K05hE9wnnnjCv3JCqVm4+nn11VeXlgAbTlYQE5oDp12p49YD4nXYYYclQ6QoxVZERKR3KSUBpYLw1FNP+TPZeRX+m2++OXnXjqumdl8P9wBxjygVzBD3etk4WRVfxuEzuz8obToiUhxJOc3pSfbYvtmeuCKadoKJ7TjtgUIkrOH2HSazWfgd25a5f3z9+vXJJ+2WLl3qm2s24yrYaaed5q/U/fznP0+GbHTdddd1nISTxim2IiIivUcpCei6dev8a1ZTxzRUWnkQyQ033ODvJXvsscf82e+wEktieeihh7rTTz/dj3POOee4Bx98MPm0HZXjq666yleM7T4/pnPppZcmY0gsfPgH8QOVffrjJIFYpl2V6K3SYgOLTxiL3h6zu+66yyd73Hd9/fXX++0w7QRT2gOFSD7/5V/+xd+rx3bJNnrRRRflxoXkk/iTrHJ/7tNPP+3uueee5NN2y5cv72iKWTb2b7Ti4Goc+y/DfLNczbwy3OoUWxERkd6j1IcQNeL888/3lQruOQOvXCGlAmKVVCqsjGPN7RiHKyoh7gfjnjWu1pAMHHTQQb7SvLkPPOqtqNxxrxVJAR0JBfHmnjr6iXmICn9fqfylxQZc3eMKDMP4nMS0L8SM7Y2kgO2LZDCr2WvaA4Xsaum2227rt8szzzzTDyepzcK2zLbLfoCEhPh/73vfSz5tF54UaAau1CG8Isd804RUNo9iKyIi0juUkoD2798/eVcciebOO++c9LUbPXq0f7WHwtCsNx4n7l+5cqWbM2dOR9IQdrIpKnck6Zbk5yHxiptN92ZZseFkhiWUjPPQQw/592l6W8yuuOIK/3rcccf516LYvu1pw2GX9/TSZcuW+avKoUGDBiXvqoGkmKScfZNdqbv11ls7kifpOsVWRESkdyglAeV+LK5AUnGgyVRRX3zxRfKuXSNNeENUXKUYkiMSAZ5YbE1HSa64wsWVKpJ5kISNGjXKv+8r0mJDRThs8klCRHnrKzHr6jaJP/7xj8m73oUnK4Mns9qV8Kw4cUKCMkI54pWu2Vdxq6yR2LKNEk+abYfxDT9TrEVERMpXWhPcuXPn+te8ey9nzpzZUSEgYaVpX5iw2md77LGHf+WhFPWSS86ak/hS0QsrG32l2WijrFkpiVbYdHTNmjV+mD0Rti81vTVZscmimGVj+yaG8+fP79jGeWU7zfKVr3zFvfTSS7knsVhHjZzk6gl2pY79F02yLWlKw0kNYsGVdcoK32MZJV0jsWW7Y9xTTjnFNxfnKbrEGscee6y/Am/btIiIiJSntASUfwhPZcCaK/IAIcN7Kp4HHHBAR4WAhJUKAwkrFUo6nnbI1Sb75/Lc+0NyydlsPmc69hAia6pHBYVEld+l8mFnwXmQSV/0l7/8xb/GTw9Nw/pKu0IQNiO1eMbNUltRd8QmS2+NmW3HcWuFkCWEYWJoJ6S499PuA+XVrhCnfYeHjHEP6Nlnn+1jz2dcCQNJBle5+D7Ne8tEDJiXcF5POOEE/8oVujDJsTiF+z+QDBn939mNNje2jGv3FVtiTznhvT1fQERERErWVrJaRattwoQJ3IDpu1py2FarzLe9+uqryRgbLVmypG3EiBEd482YMaPt448/Tj5tN2fOHP8Z4/A5/Uyf3zFMO5wOvxdPpy+wmIddHuIUI64LFy7074k147z11lttteTeD2tVmxObcFxiQhfqrTEbO3bsJjELtzsTfs53DDEhBgznNYxb1nfYJ9h3GG77CIsv2zXbeNp89IQ4BuEy8JnNB6/heHS2XCyPjUfZiMtPX9UdsQX9sG2PVysvIiIiUr5+/KkdoEU64SoB9+hZ81HD/VT2oBi7D5LmbFyNoMlpXxDHhqubXHnjyj5X3rn3M7wyo5iVixi/8847HVecq44yw1U6rshRlniQWrzdSdex/R122GFu//339/08KIx+xbh1/HrRA+7LLze4H51+ejKk+61YvtytWrnSnXf++ckQgWIvIj3Cp6EiNeGVhPAKgkm7Ymfj9/YrCvVikxWHvhyzZuEqaHhVtMq4ImflgStz9t6u7snmI67hdqj4tpbpF0xrO/OMyW0ffvhhMqTn8FvjvzOulN9qBYq9iPQUXQEVkV6H+wAPPfRQfxVUD34SaU13LFjgXn7pZXfLrfOTIT3vomkX+tc5113rX/sqxV5EelJpDyESESkL//pp9erV7re//W0yRERayUcffeRumvtLd8GF2U867gkkP3968UXfLLSvUuxFpKcpARWRXon/D9kbnjQs0hfdf++97pv77uuG7LprMqQ8Rx/zfTf/lnlJX9+j2ItIT1MCKiIiIpXyyMO/cV8f+vWkr92a1avd7MuvcMP23Mu/nzp5ihuy81fdIQce5PvB1TuajzKMK2mMb+P8edUqP95Jk07Y5HuhYcOHuxdfeCH1s75AsReRnqYEVERERCqD5GPt2rU+GQn9/Nrr3J133OH/V/OSxYvd5bNnuSeXPu37b5t/qx+Hq3c0H+X7PFl1wqSJ7oWX2/8H7Pnnnue/d8PcGzf5XujrQ4f611UrV/nXvkSxl7JwEiILJymsMzyR2YY9sGhRxz3DzWQnVdLwmc1vuKw33nBDx3Des1x9kRJQERERqYwPPvggedcZD8TZd7/9/Hv+Zcd2223nm4nutvvu7v333+8Y/sNTT/HvSaL4nPFo2klilPW9EJ/jgw/W+de+RLGXMpB8LbjzjqRvU5ykCF9x/MQJ7h/PO9ddefXVbsLEiW74iBGZyV8ZuMp/+qk/cvcuvD8Z0hnl/M577vbvn31+hX8F28Exxx7rP+P9ylde8YloX6MEVEREREREehxXLkm+SNCy8BlJWtqVcBJRex25z8imXUG8dMbMTollmoNGjfInbuIHa22/w/b+M/DwLZ443deanSsBFRERERGRHseTji35AsmZNUkNk8nxRx3pHnv00aSv3br3O18ZP2L8+E3GKQPzzIO6QmHT2jCZPOq733WLH3s86WtvmhtjHJqo9yVKQEVERKQyBg4c6F83rN/gX5tl4MDtk3d9h2IvPYnEbdCOOyZ97biSuOadv/rmtjMuvjgZ2n71cO1773UkbCSnJKUhrpTy0KqycY8zVzENy0VyzHLQRPinl/0k+aT9Su3DDz2U9DmfaJI4hwZuP9BfBe1LlICKiIhIZVCpHDRokFu9+s1kyEZffPGFf+WJq4ZhNhxfbvjSv4ZJlF05yfueseZyw4YP8699iWIvPemDdZ3vMWZ9c38wVw0PHz2mY5jh/mG7Msh9weGV01DZzVfjK7EkpCSZLAdJdJwU05w4vLqb1vyYZLsvUQIqIiIilULFM74iwANH3nj9df9+v5H7+FcqfAyj4z3N4HhaK8495xxfmeV7dgWC7zEs/l5o9ZtvuqG77ZZaSewLFHvpKVzpi3GPJFcOrQuTTK4U8m+BECd9obLLS3j10/CApHA5QtacOC9Rjq8M93b92mqS9yIiIiJNx9Wysd/6tvv1ww+VXrnkXyZMv/hiN278EcmQvkWxl57EOg4f3sNJCB5KROLJVUKS1DAJ5STGDjvs4JO4+AooCR3NXbOeRNtTOJHCfZ08QMj6Tz35hx2JJw9ass8My819o2dMmbzJdsVyc4WXp+L2FboCKiIiIpXCv+O4eMYMd/55/7NT082edseCBf4KXF9OgBR76UkkYWFzVO6ZJHkjEeUqYZxk8oAerqLHw0HzXD4vG/PCw5Tsiib9NLNlGejSrpDSsoDvpJ3UYbnj+0J7O10BFRERkUriSsLrr7/u7rj7ro7/EdlTaEL6+6W/L+W3WoFiLz2FJI2HDm3OFXaSWBK3sq9+Gq56FvlXLPWwnZGw9qWrn1ACKiIiIpX1xOIl7n/9rw/cj04/PRnS/ahMLn/2OTd56plKgAKKvfSUuCluI+ImsM2yuU2AOfHCE5/tf5v2JUpARUREREREpBS6B1RERERERERKoQRURERERERESqEEVEREREREREqhBFRERERERERKoQRURERERERESqEEVEREREREREqhBFRERERERERKoQRURERERERESqEEVEREREREREqhBFREetzzzz/vrrnmmqRPRERERPoqJaAiUtgTTzzhhgwZ4vr16+fOOuusZGhnb7/9ths5cqT75JNPkiHOHXjgge6dd97ZZLiIiIiI9C1KQEWkEBLHk046yV144YXu448/dosWLUq9qjlhwgS3YMECt8022yRD2t18880+Ab300kuTISIiIiLS1ygBFZFC3njjDffZZ5+53Xff3SeX++yzj1u2bFnyaTsS0uOOO87ttddeyZDOSEKffvpp3yRXRERERPoeJaAi0i1IKklIp0+fngxJN3nyZDdr1qykT0RERET6EiWgIlLI0KFD3YABA9xf/vIX3xz3pZdecocddpj/jP5TTjnF3Xfffb4/z/777++eeuopf6+oiIiIiPQtSkBFpBCa3d57773u2muvddtuu62bOHGiO+200/xnZ599tps7d+4m932mIZEFCayIiIiI9C1KQEWksHHjxrk1a9a4trY2fz8nCef8+fPd4MGD/WeYOXOm23rrrX3Hg4pilqS+++67/lVERERE+g4loCLSZa+99pp75JFH3OzZs30/CeeVV17pnnnmGZ+gTpo0SU1tRURERKSDElAR6RLu+7zooovcnDlzkiHO/fa3v3UjRozwT8GliS4eeugh/yoiIiIiogRURLrk+uuvd0cffXTmv1ypZ6eddkreiYiIiEhfoQRURBr2xBNPuLfeestNmTIlGdLue9/7nnvllVd801zuDcXYsWP9q7H/Acr/ERURERGRvqVfG08TEREpiKa3hx9+uHvyySdTn3p7zTXXuKuvvtq/5z5Qa4prSEwXLFjgXn755WSIiIiIiPQVSkBFpFRDhgzx/7LFnporIiIiIn2HmuCKSGm4+slDipR8ioiIiPRNugIqIqWgae6DDz6Y2XRXRERERHo/XQEVkR7Hg4e++OILJZ8iIiIifZyugIqIiIiIiEgpdAVURERERERESqEEVEREREREREqhBFRERERERERKoQRURERERERESqEEVEREREREREqhBFRERERERERKoQRURERERERESqEEVEREREREREqhBFRERERERERKoQRURERERERESqEEVEREREREREqhBFRERERERERKoQRURERERERESqEEVEREREREREqhBFRERERERERKoQRURERERERESqEEVEREREREREqhBFRERERERERKoQRURERERERESqEEVEREREREREqhBFRERERERERKoQRUREREREREStGvrSZ53yX9+vVL3omIiIiIiEir2cyUsCGbnYCKiIiIiIiIFKEmuCIiIiIiIlIKJaAiIiIiIiJSCiWgIiIiIiIiUgoloCIiIiIiIlIKJaAiIiIiIiJSCiWgIiIiIiIiUgoloCIiIiIiIlIKJaAiIiIiIiJSCiWgIiIiIiIiUgoloCIiIiIiIlIKJaAiIiIiIiJSCiWgIiIiIiIiUgoloCIiIiIiIlIKJaAiIiIiIiJSilIS0MMPP9z169dvk27kyJHummuuScbaaObMmW7rrbfuGOeJJ55IPpGuWrRoUUdMWR+ffPJJ8slGRcbp6rp57bXXOsoBr/TH3n77bTd//vzMctFTisZmyJAhHcv9/PPPJ5+04zt8ltadddZZyVib4nsTJ07sGJf3abEJf5/XMuMTKjq/hnXK8lt862H6Nq51cRkrUpbKVq/sFolbV8oQseHzWFXKS56iZamR9c00WVZb9nA75XusH4sJ6ytWxbht7n6RGFiciZ8J48E2RxkjflWUtx8pEh+Wi3VLHMIYNIJjX9p3i5SZVqvTPLF4iRuy81dTu18veiAZy/n3w/bcyw8/adIJ7qOPPko+2Wj25Vd0jHPkuCP8tFvVmtWr3R0LFvjluPGGG5Khxa1YvtxNnTylI16hME6Mw2+1KpYlXr40f161yseSZWbZL5p2YWoZYjymeciBB/kYVh3LYOvZ1ifLUATftXJgXbjNFI1ZS2gryauvvtrGz82ZM8f3v/XWW21Tp071w3g1fL5w4UL/nnEmTJjgx1mxYoUfJo1bsmRJ27x58/x74jh48OC2sWPH+n5TZJyurpuPP/64bcCAAR3TZxr0MzxEOeB3w3LS04rGhvmlDIPxmUfrB8vEsLSO72dhmS1+vI4YMWKT2PB9pmPzye8yjq2LMhWZX2MxCb9TTxxHph0qWpbKVq/sFolbo2XIYsHnIcZlHvicjveMU9Y2VVSRmNgyFlnftl2w/RKDcBz2V3zG98HvhdNFVeNWr2zl4bssJ98L91d2/OUVFtd431cFtl2E5SVUJD6sZ8oX43RlGfndtO8W2TczT9bfKnWa6RdMaxv8dzundh9++KEfZ8nji9tuv+02/375c8+1HXzAgW0nTpzk+80vrr++7YGFi/z71W++2XbmGZP9NBi/FREXlpNlYNkawXf3/sae/nurVq5Mhrab9bPL28Z/Z5yPLZ39jsW6lbBuiU9cFmKUB5aTV1BOiE/a94gNn7VK2WG5bD55tfkvsj6JA8tpHd8zjcSsFZSWgCLtAGEHDjs4hhUCWAWEnbZ0TXgwBOuAmIaKjNPVdUMFgYN/iAM5w2N2oM+qSHS3IstNGY3HY/7Dykha5cgqvVkYP6wUwpY/jDXxjeM3Y8aMLlWkNkfR+QXxYtnTEqc8xNoqxWkaKUtls1jEZbdo3BotQ1YumE4oXhcgRnllsWyNxKTI+mZaLF/WfoPx4+/Ytm6JapXjZrFpZL9osYvjDLZPW27DtPmNtPGbpeh+pGh8GKfR/SZxIo7sm+LvFtk3x+WqFeo0VGitkmuo7JJAGkssDYlVWFmGJaiGCjjjhNNpNZZgNZKAkjSQhMSJJ4gz0wvjbXFqNMltNuab5Uw7GRGj/MQJGctLLNLiZJ9VPQFl/uL5tzITbw9piF287ZlGY1Z1Tb8HlCYr2LBhg3+dMmWKfzXbbLON22effdznn3+eDJFG0ewo9M4777ha5STpa1dknK6uG5ooHXfccUlfu6OPPtoPb7Z6y00ztVoS4AYNGpQMacf8P/XUUx1N1ojNgQce6N+bpUuXbhLDEOPvtddeSV87m8YXX3zhX0HTrVdeecU3NTPME/NQpqLzS8wmTZrkrrrqKjdu3LhkaH2UB5aLpnZZZaPKZSlL0bg1UoZowke5iGOBeDvFYYcd5j777LOkr/mKxqTI+mYbPOaYY9yYMWPc9OnTk6GdMf7OO++c9LWrJQk+Jn/60598fyvErSiapN5yyy1uwYIFm8QZ7PfYf4f2339//2rH4mbr6n6ku11//fXuggsu6KirhIrsm7t63GwWmn7eMPdGN2TXXZMh7Z5ZtswdedRRSZ9zx0+ckLxrt+79de6YY49N+tr96PTTk3fttttuO7fb7rtXpoyVgSa7Dz/0kLt81hVu72HDkqEb1ZIT/xrGmzh9c9993e+X/j4Z0hpuvWWe+8HJJ7tBO+6YDMlG+WE5Q8OGD/evX375pX9tRQeNGrXJemYY6pV7mrSvXbvW/fSyn3Rq6m56W8yanoBaBb5///7+NQ3jFKlsMx6VV+6zsPsx4nv1+jK7jwazZ8/2r7Ei44TqrRumRwVujz32SIa02712EGI4lYwqyFpu22GsX7/evxrmH2+88YZ/TavkUfk7/vjjk75ibHugcmymTZvmBgwY4CZMmODjRWWaik9ahblsafNLhZH5JZFgPtkWia2Nm+Wuu+7yryT2VDy5Vyr8TquUpSLS4la0DPHdn/zkJ+6KK65IhtTHuqD8VFkck6Lr+6Fa5Y5K/7DaQd/uxYvvFWX8MLGFxfvf//3f/WuaVohbmh//+Mc+jiSixIPtsN79o+zj2G7jkyDN0tX9SHei/kDZik9Umq7um1mGInWaZiARiiu53GP2pxdfdOPGH5EM2YiElfvQMPOyS/1rHtbnYd86LOnr/W6a+0u37377uUX3L+y4by+8f9TqGPF9fF8f+nX3xuuvJ33Vx72ZJE/xiYlGbFi/wW255ZYdCVtvYet21MEH+9csjz36qH998YUX3IyLL/b3eta7v7OVY1Z6AmqVAHbAHEw4e8iBMq3yBSohHACOjc6spbn00kvd008/7T7++GPf4ZRTTvGvfR0H0sGDB/uz4sQoLTEvMk6oyLpZt26df2UDSVOFM6F5y7399tv718WLF/tXw44WWSdOqIxQ6c0q11m44hVvD7vssot77LHHfKwPPfRQt7y2o7/55puTT5srbX4feOABf4af4Z9++qmbN2+ej+3ZZ5+djJHuySef9Mu4cOFCvz7YN4TfaYWyVFRa3GJZZYiYkJjGV7DysE7OOeecpK+a4pgUXd+PPPKILy8kqmvWrHErVqxwL730kr8qaskKnxODEPsvbLXVVv41TSvELcb+i3IzfPhwnyBxLCSBuuiii1IfvGTYx11cq/RURVf3I92FsjNr1iz3q1/9Khmyqa7smxup01TF47WK8egxY5K+jUg6Dh89xl/hI0Gt94AYktX3a8fOI7/73WRI70Y8OLEzdOhQd8aUye6Fl1/ycfzljXP9lVEMHNhex3jmD8v8q+GKcta+r2pIkubfMs9dPntWMqRrnnv2WffDU3tfnZ11y0mItCvgoXsX3u+eXPq0u/Lqq32rO05AXDbzkuTTdC0ds6Qpbin4uVpFoOO+zwEDBvj7VLgnIgv3SRS9j4xxmZ6xe1pkI7unhq52EEyGdlZkHBRZN3ZvDq+hesMbudepu2Qtd60C5OeJz8E9UgxjvCzcB5R2T1ketgPuJ0qLOb9J2ebzcF6aKW1+s9Yr887wvPIUYtoWd/tOvTITDy+bzUe9spu3nkNpZYjtLZx+kX0c02BaVdZIWYqHp8Wc7YPhtp1YnOz4wO8QE4Zl3fNYpbgVLVvIKhN27E1DDIh/VWSt+6z9SNH4MA77lSJY9+Hv87207za6b26kTlMVWfcvGnsYCl3W/Wvg3k8eXtTKGrkH1O7Pi3GfHx3sfk86izEx4vNWuVeWhyiF92Zy/2ejD8Zh2SlnWVrlHtCY3Rebt12k4XvEkGXO+m69mFVd6VdAJ0+e7M9S137bn9XkbGHWmXyas3BWMb7/g6Y4YWdNixif6XF/lJ3xlc6IC2dsOUPOFYc0RcbJWjexvKbVqPd5mbKW+7777vP34dEslOZVdu8n42fh7P3o0aOTvmK4gs+VLc6qh7gSxtUcmlxyldDmpdmP8s+a3zTjx4/3r3ZVqx72CXYlwb7TSmUpT9G4xWWIMjd37tzM+xzTUHboijSnb6a0mGzO+ra4vfvuu/6VmNWSE7/f4phx3XXX+e2cK6NpV6FbJW6NoJloLXFL+jaiXNHclX1L1TW6H+kqawVTrzlyo/vmosfNKuGq5Yb163Ov3tDs8sabfumv9tk9jTHuaRu5z8jUZrx9DVdBrRUVzZ1vv+tOf2/scd8/xv+rEe7n4/NDD6tOU2Wu5ob/GoSOYXbVe3OagHIF9dZ5890dd7ffhtMKsuIRu27ONf7+3/ie6nooFz+9/Gf+/QcffOBfQ60Ys1jT7wHNwgGA5iyN3OfGwYB7gGhKdPLJJ/sKh2yqyD0+eeM0sm6o3A0YMMD98Y9/TIa0o5/heU0QmyFtuS0ZspMmPKyD5qE0b0tDfFi2IomZ4STKqNoOPC0eVA4p18yHzQuVyXPPPTcZo3xZ82tNlu3gaqwpUSNJIvEjQbBptlpZSpO3nkNpZej222/3Jz/Ck292ko338f8oJLHg80buFW2GrJgUXd+UER4eFrKTmmHzWpJQtl+2Y2JCMkATy1irxC3LTjvt5F+tibEhFsQtRpNW7hm1mFVBd+5HuoJyceWVV3ba1tj2bPuzk96N7Ju7UqepgiW1+lRa89tYXgJCxXxl7ZgZP5Sot7PmtfH/9Nyi/xadmteS3NP8cs07f3XPPr+ilnCs800wN+d+yrLQ9PbOO+7olIhxDyMd74v8v1SamU4+c8om9x63OpZ9+IgRdZveZiFppRwMHDgwGbJRb4hZJRNQEsnf/e53HVdAQGWBDlQgws6uCHBmkZ0/32ulM4xlo4KFvCt0WePUWzdpuFK4bFnn+xvoz7uC2Cz1YsPyc1/xwoULMxPM+++/3z81sShiR6UxjAf3R1sFMu1piZxgoTLdDHnzS0xG1Ha49kAhQ0Uy62pTFtYFlbswzq1UlmL11nMorQyxn4v3fXaSjffhFSxix1VFrt5bYkHZ5R/iV0m9mBRZ3+zzmY5tu7Dvp23HjHfiiSf6aYTTQavELY8tMw9nCpGkx8vLcpF82nbJ8sfjNEN37ke6gm0p3tbGjh3rO95bnaPovrkrx82qeOTh37gJk+qXiawHrfCP85c/+5ybc921yZD2q6FpT/nsbQ5NHrZEEh/i/s6spP6JxUvc3Xfe5Z9EXCWcYCBBDjuGWeIcdtzvSMf7884/P5lCutmXX+ETKUvSKEdTJ1f/JE1WPAzlmxMQ4UkEHtYVn4zIQyx4onB89bRVY7aJ2s60FNwnwc/Vu6eGeyMGDGj/5+pxV++eKcapVUb8e36P+zXse1n3+fR2FnfujeE+K7u3LlwPRcZBkXVj9+KE97gwPb5n98ZwbxX9aeuT7/H9Mu69KrrcYFzGC5cjC+MwrVhabJgmw+KuVslKxtg4jt0PSNy434jhZSsyv7acNr/0E5NwueNYsExM2+JGvFkXvIYaKUtlyyu7ReIWyipDMZtuiJjZ/WhxV6/slqlITIqsbxuH+/B4b9tHvB4YznSYPuPGqhy3emUrjokNYztDHDfixLEyXk66tNg0Q5H9iMmLj2GZGYd1HON7WdM27I/oQlaGbR6t7DHcME2mzXhxF66zKsq6x4zhdh8k96rZ/WrcCxjiXkbubWTcuGv0nriqYJmY/3hZQTzi+2BtmN27yP+CjMcBn/P/QsN7QVtV2j2gLB9xs3uAKTPc4xqWCeuIQ4x481kr3ENs96vGnd33izgelAfbnkAZIIZhWWg0ZlVXSgLKTjve8dqBMWQHkbQu7aARs4MBO3sOCEUOSr0dB90w/ryPD7JFxim6buLEwoSVO6YfJxYI58G6nlRkucFnlCkqZvUqDHzfToLE4thQLu234y4us5RtKs58xmtYwSlLI/PLMobzG8c1jgVxtfEt1qyfNEXKUtnyym4jcUNeGYrZPs8Qx6zKLl1WTMvWSEyKrG+G2Tpg+ePtwz4jrmnHnirHLa9sgWVl3uN9kw1n/DhuFs+0Lt5Wm6nefgT14gPbTsIuLAeUC2KVt93xO3Qxph3OY1j2mN/4d60Lj5tVRaU/7Z/nW8JplV/ex4mBJWppXas+OCVcZutCaQkobDjjx0mFJSIkJ2EC0spYRrpQnHBRBiyGcReXpfjzeNpVYolyWheetEhLQCkDDKOskFDGZaGRmLWCfvyp7QxFRERE+iyaJPemB0+JiFRVZR9CJCIiIlIGHhJ0wAEHJH0iItKTlICKiIhInzV//nz/L0T08EIRkXKoCa6IiIiIiIiUQldARUREREREpBRKQEVERERERKQUSkBFRERERESkFEpARUREREREpBRKQEVERERERKQUSkBFRERERESkFEpARUREREREpBRKQEVERERERKQUSkBFRERERESkFEpARUREREREpBRKQEVERERERKQUSkBFRERERESkFEpARUREREREpBRKQEVERERERKQUSkBFRERERESkFEpARUREREREpBRKQEVERERERKQUSkBFRERERESkFEpARUREREREpBRKQEVERERERKQUSkBFRERERESkFEpARUREREREpBRKQEVERERERKQUSkBFRERERESkFL0mAf3kk0/c/Pnz3ZAhQ9zzzz+fDBUREREREZGqKCUBPfzww12/fv026UaOHOmuueaaZKyNZs6c6bbeeuuOcZ544onkk2y33367+/GPf+zeeuutZIiEFi1a1BFT1gcJex7WAePFXnvtNb9OmA7TO+uss+pOC/w+Jwf4Hq9p673ReewuRX43nH+WP+0kR1dj8/bbb/uTJ1nbA4rErwwsz8SJE/180PGe5Y51dV2G2z7TJjaxqsQi1Og6TCtDxIjP0jrKkmE8pkV80rbRGONauaxCrEJFygnli89snLTyxrCwTGSNU2/7bNWylYZls9hal3csbXT6ZbF1bx37iFCRddaVOkVf9sTiJW7Izl9N7X696IFkLOffD9tzLz/8pEknuI8++ij5pB398fetu2jahclYrWPN6tXujgUL3JHjjnA33nBDMrS4FcuXu6mTp/jlJ16h2Zdf0RFLps86aFUsS7x8af68apVfVpaZZadMxGUIrRYblsHWMx3vWdZG5JUVlv+QAw/yn2XFrCW0leTVV19t4+fmzJnj+2uJYtvUqVP9MF4Nny9cuNC/Z5wJEyb4cVasWOGH5eG7RcftS5YsWdI2b948/57YDB48uG3s2LG+Pw3jEMd4HNbHgAED/Pr6+OOPfTdixIhO6y8Nv8/0bB4oC0zH1jMancfuUuR3GYf5Zb7B+CyP9aOrsQHj8LtM07aPUJH4lYV5te2LV5aReWF5TVfX5YwZM/z0LH4Wl3jaVYlFqMg6rFeGWAaGpXV83/Bd4sTwvLhaGWS+mDZltEqKlBOWgbjZeCxHXN5YLsoOw3jPNNLGYRjrieF08fbJ/LDu7HM7nqStzzLVK1tZ4vLE8mepyrLGWG/hMtCF20yR/QHLZP1Mr5E6RV81/YJpbYP/bufU7sMPP/TjLHl8cdvtt93m3y9/7rm2gw84sO3EiZN8v3lg4aLUadDx/VZDXFhO5v8X11+fDC2G7+79jT3991atXJkMbTfrZ5f7z4gjLG6r33zT97cSloF5j8tCjGUjJraMLDMxiL/XirFhuWx+eR3/nXF+GWzbqSevrDC9MB6MWy/WVVVaAgp2+vEBzg6sYcUsREWAAwoHjXrsIKoDS2fhwRjEKasyYhWztMog64b4Mo6xCkAe1h3TDFFhDKffyDx2pyK/axX4EPMezn9XY2Mos4wbbx8oEr8yMI9h5Q823+F225V1aRVNXo1t+2FMqhKLNHnrsEgZItGI912WOKXht7KW27Zj4hWWySopUk6ISby+WeYwcYynY+shLKtFts/42AN+q17ZLUNe2cpCmQu3pyzEiRg3Ov0ysJ7j9Rsqsj+I16vtV/iupKNCG1fwqfifecbkpK+9P0RlmYpxKKyIG6Ybj9dKWJ5GE1DiQBISJxOGeJBohRi/0SS32UiwmO+0kxExyk+ckLG8xDaMU6vFhvKRljSyXHbCJk+9skJsw3gQQ2IUb4+toOn3gNJkBhs2bPCvU6ZM8a9mm222cfvss4/7/PPPkyHSKJrqhd555x1XO7AnfZ1df/317oILLuhYL6GtttrKvy5dutS/4r333nO1A3nSl27rrbd2r7zySqfmlLWKkTv66KOTvsbmsTvV+12a7TGvgwYNSoa0Y96feuqpjiZ8XY1NEUXiV4YDDzzQ7bXXXklfO4bhiy++8K/oyrq0uO2yyy7+FWz7Y8aMcQ8++GAypDqxaETRMsS+z+JpiEtXtoOzzz7bffbZZ+5Xv/qVj2MVFSknNK887rjjkr52xI3hJp7O2rVrXS0p6VRWi2yf8bEHhx12mI9jqyE+lDmaGYexSnPRRRe5BQsWJH3VwTZ+yy23uJ///Oe+WW1a8+wi+wPVKRpDM9Mb5t7ohuy6azKk3TPLlrkjjzoq6XPu+Imdj23r3l/njjn22KSv3cQTJrmDRo1K+trVKuObjNeb0WT34YcecpfPusLtPWxYMrSzLbfc0i19+umkr937tf3YqIMPTvpaw623zHM/OPlkN2jHHZMh2Sg/2223XdLXbtjw4f71yy+/9K9otdhQ3uP1bNuA5TlZ6pUVmvFyfBt1yMZlJ4bf3Hdfv322mqYnoHZQ6d+/v39NwziNVDBZQXbfCImU7vdox0Ha7iWbPXu2fw1xTxoH77hCZxhOxY5pEFMq1o888oiv5OaZNm2aGzBggK/s8R0qRFQc0ip89eaxp2T9ru0w1q9f71/N7rvv7l/feOMN/9rV2BTRSPzKZtvv2LFj/WuokXVpCWxcyRxW2wlTwTRVjkWWomUoTu5BYnD88ccnfcUQlwceeMAn7yeeeGLl94NZ5YThJH977LFHMqQdcWM4yxmi7JCo3HXXXe7JJ59Mhrbr6vZJueyOk0hlIwbgBMekSZP8fY/xtgXixbE1rew120O1ihjY/kmSd60lRPE67+r+oNE6RV9C4hknBtxj9qcXX3Tjxh+RDNmIhNXu55x52aX+1aRVoh/5zSOp0+mtbpr7S7fvfvu5Rfcv9PfscS9jfP/o9Isv9vVW7vkj1sTz4hkzMhPWKuKeRZYhPjHRiA3rN/iEMzxp0RtiY/do1kua65WV1W+u9q9fHzrUv5qvD/263z5bTnIltBT8HM1jQDOYqVPb7wHNakaGWkLkm8sUaUZG8yGmx3QZn+8ybYbxvi+zJlx0NM2Km/oRL2JlceZ92nohjjR5svVWZL2A32M90rF+0tSbx56S97ssL8PjeaZZGMPDZn5djQ1sHrKawPF5vfg1A3FIKyd5MU1j8Yyb27GsLHOoqrHIWoeNlKEQw4ldFr6bFnvbDzJ92w9aucz6rWbJKyf2WTgMWcNtOpSLtOa0Xdk+y9wP5bFlbqSJLMtLGWAZ+G4tSUs+aUdZCIc1Ov0ysI5oKs36Yv5Ylni9EZtG9gfEhXEb2T/3dTQdpGlgzJoW0tE0kP48NCtkvFZmy1ykCaiNS5NJmh7TXJI4pjXHpJ/hrdickuWiya01qeV9V+5LJDZpcW3l2IB5rhePImXFmijHsoZXXekJKAcQOyDaASPvQMABkgNQEVbxCisMTJthlvj2dVRI7GDNgdgQnzBuHPDTKrfEk3XGeiGuRRMAKjuMaxXAONEIZc1jT8v6Xav82DyzLAxjvFBXY4N6FcxG4lcWlpf5yVtHRdcl07LxLEliu2dfkVZxrloskLcOi5ahENtkWiJlmF7aNsqweDixZ/xGymSZ0sqJxTPcLyFrOBhm5SI+bjS6fRL7qhw3bJm7kiCy3Fb+4v0an5muTr8srAvmMd7eG90fNFKnkHZ596SBCjbJAV3ew2GoXMeJV6tpJAHNSgxIwuNEnIcykXBYHPPiXTWs1/DkQ1cSUJaXcpamlWNDIsly5W0XKFJWlIBuhkYPcBxI0ipgTCfsbJq80h9XTNIqZH2ZVWYstvTHFa20mFnCYfHl+0ynXiWNCoKdubZKIN/LqwTE81iWtN8N55kKMuWMOIQV2K7Gxtjvpm0fXYlfGZgP5q2eouvSkjLGZXnZ/nkfViirGgvkrcNwXrPKUIzlzEvamVbafi1t2wW/lza8KuJywrqm37YpY+NllT1iTYzDExcMa2T7ZNp566ZseWWrCDsBYcvPdOJtZnOmXxa2iXAeG90fZNUpJBsV5yJXLS0xy0swmU69injVdUcCSsIWDg+vkBEfEpZ6yXzZbLnDjmF0LE+o0QSUJI0HXNkV1FBVY5MVjxiJc5GEuUhZsSvBMb5LTFpN0+8BzcL9iMuXL++We7u43yN8uElfFz/oZNasWe7KK6/094pZx71DdLy3/6vGPTncj2PfZ93UDub+u9yvleWqq67y96Dx8Ae6m2++2d+zc+655yZjbCqex7Kk/a7Nc217cZ9++qnbf//9fRy4/8h0NTZFdCV+PY0yMWrUqEL3jhVdl0yLe/eI85o1a9y7777rapXLTvckVzEWRRQpQyH2f7Ukqkv7Lb5D/GLMw1e+8pWkr3rickJ5IAZ//OMfkyHt6Gd4VtljOXnITKiR7ZPjBfccXnHFFcmQ1keZYFvafvvtfT/Ld8QRR3Ta59tw3qf9n+Mq4L7mnXbaKelrbH/QnXWKvmTJ4sVudC3u9cQPG4pxj2D/Lbfc5OFGvdnAge3bG/fJhrbov4W/19FcXdsPjdxnpH9PfO64+y7/+W3zb/XDqmz+LfPcnXfc4e9ZtO7FF17wHe+L/L/Uy2Ze4iafOWWTe4/RyrFh2YePGFHoftUiZcWmw7YUevmll/2DiFpNJRNQHibwu9/9zh9MDA8XoAOVuLCbPn26H56GygUVDyrL0s4eRjF69Gj/apX+sBs7dqzvwviGTzo1xyZPs8t7ulfa0wZPPvlkXxHPEs9jWer9LmXzlFNOcQsXLuyUHHQ1NkV0JX49ie2QSmCYGPJwl6xEuyvrkgfFXH311e7hhx9OhrSrWiy6IqsMhe6//37/NOquGD9+vH+YWJxEkJR+73vfS/qqJ62cUMaWRU/3oz8se2mYVrisRbdPvnfppZe6++67zyc0YH3NnDnTv29VLBeJmpW3eH9Phzlz5vj3RU8alY19TFg+iu4P6tUpJNsjD//GTZiUv72h3oNWFj/2uH9Cal9y6LcO868k8SGeGBwm9fED6kjE+Dwe3kycYFjzzl87dQy7d+H9mwznQTp0vD/v/POTKaSbffkVPvm05IpyxAOHTFVjkxUP8+tFD/ikMnwoEw9QihNMU6SsECOepr9q5UrfD+L1+l/+4g49rP37LaV2sCmFNaeq1ySRpjM0n2LcuMtrjgZrssdvWJOces3cejuLO82WLCY0w6u3Hhgnbq5nzcCIp02L9+F4Nk7YBIrfZpg1fWI9sl6sKVVX53FzNfK7jMt4lM2wSajpamwMw/gs7bfrxa9MNi9xRzM4FI1pViwYTtyIM9OKVSkWsbx1iHplKMQ4xC4L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\"\u003e\u003cbr\u003e\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003ePerformance of ECDs\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eAs show in Figure2 a, ECDs are typically composed of two transparent conductive layers (substrate), EC layer, an ion-conductive layer and a counter electrode layer. The cyclic voltammogram (CV) and ECDs of the P1 are shown in\u003cstrong\u003e\u0026nbsp;\u003c/strong\u003eFigure S3. The oxidation peak of P1-a is 0.80 V, and the reduction peak is 0.61 V. Photographs of the devices are shown in its neutral and color states. The device operates between 0.8 V and -0.1 V. The P1-a device displays blue in its neutral state and becomes transparent in coloring state. The oxidation peak of P1-b is 1.18 V, and the reduction peak appears at 0.95 V. P1-b is blue in its neutral state and similarly turns colorless in the bleached state. The oxidation peak of P1-c is 0.91 V, and the reduction peak is 0.70 V. The oxidation peak of P1-d is 0.76 V, and the reduction peak appears at 0.54 V. P1-c and P1-d manifest as deep black in their neutral state, but become semi-transparent at a voltage of -0.1 V. The oxidation peak of P1-e is 0.99 V, and the reduction peak appears at 0.72 V. P1-e appears yellow in neutral state and switches to green in the colored state. The oxidation voltage and reduction voltage of these devices are low. These copolymers undergo reversible electrochromic switch from a strongly neutral black to a highly transmissive oxidized state within a potential window of less than 1 V, representing an ideal parameter for low-driving-voltage device applications. The EC performance of the device in neutral state is consistent with its absorption spectrum in solution.\u0026nbsp;When an applied voltage is present, the ECDs transition from a dark to a light color. Notably, the P1-c and P1-d ECDs exhibit dark in its neutral state and only partially absorbs in the visible spectrum.\u003c/p\u003e\n\u003cp\u003eThe spectroelectrochemical behavior of P2-b is displayed in Figure 2c. In the neutral state, P2-b shows strong absorption at wavelength around 681 nm. When P2-b is oxidized (increasing the applied voltage from 0 to 1.4 V), the device gradually becomes transparent due to the oxidation of the polymer, and the absorption peak strength of about 681 nm gradually decreases. When the oxidation voltage reaches 1.4 V, P2-b exhibits weaker absorption in the visible region, making it appear transparent. In the process of oxidation of the polymer, absorption diminishes in the visible\u0026nbsp;spectrum, with a polaron transition in the near-infrared (800-1200 nm) and a weakening bipolaronic transition in the near-infrared. When fully oxidized, the resulting dual polarization absorption peak exceeds 1600 nm, allowing for effective reduction of visible light absorption with high transmittance\u003csup\u003e5, 6\u003c/sup\u003e.\u003c/p\u003e\n\u003cp\u003eTo measure the efficiency of ECDs in achieving optical modulation with a given voltage, coloration efficiency (CE) assessments were performed. Coloration efficiencies (\u003cem\u003eCE\u003c/em\u003e) were evaluated by dividing the change in optical density (\u0026Delta;OD) by the injected charge per unit area (\u0026Delta;\u003cem\u003eQ\u003c/em\u003e) (eq 1):\u003c/p\u003e\n\u003cp\u003e\u003cimg src=\"data:image/png;base64,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\"\u003e\u003cbr\u003e\u003c/p\u003e\n\u003cp\u003ewhere \u0026Delta;OD is defined as a log of the transmittance ratio of the bleached state (\u003cem\u003eT\u003c/em\u003e\u003csub\u003eb\u003c/sub\u003e) to the colored state (\u003cem\u003eT\u003c/em\u003e\u003csub\u003ec\u003c/sub\u003e). The variable \u0026Delta;Q denotes the injected charge, which is determined by integrating the transient current profile. This integration process is detailed in Figure S4. As shown in Figure 2d, the coloration efficiency values were 762,1273, 887, 728, 548, and 229 cm\u0026sup2;/C for P2-a, P2-b, P2-c, P2-d, and P2-e, respectively, which is favorably compared to the other ECP-based systems. The maximum coloration efficiency reached an impressive 1193 cm\u0026sup2;/C, surpassing the previously reported ECDs coloration efficiencies (as compared to other work, see \u003cstrong\u003eTable S1\u003c/strong\u003e). High coloration efficiency, which means less charge is converted into greater optical density variation, is a desired parameter in ECDs. This performance is highly valuable in EC applications, as it means low energy consumption and high overall energy efficiency.\u003c/p\u003e\n\u003cp\u003eTo investigate the electrochemical behavior of P2 devices, cyclic voltammetry (CV) tests were conducted. As shown in Figure 3, the oxidation peaks of these device are between 0.5 V and 1 V and the reduction peaks of the devices are between 0.2 V ~ 0.5 V. The lower redox voltage not only increases the cyclic stability of the devices but also saves energy. In the process of oxidation, the color of all the devices switches from black-to-transmissive. We find that these devices exhibit reversible electrochromic transitions from an intensely opaque, neutral black state to a transparent oxidized state, all occurring within a potential window of less than 1 V, a desirable feature for low-voltage device applications. This enhancement is ascribed to the bipolar TEG side chains\u003csup\u003e35, 38\u003c/sup\u003e, whose synergistic effect enhances charge transport and increases ion diffusion rates, resulting in reduced driving voltages required for ECDs.\u003c/p\u003e\n\u003cp\u003eCyclic stability is one of the most crucial parameters for evaluating ECDs. However, degradation of their optical modulation is typically observed after several hundreds or thousands of cycles, and lifetime is also crucially dependent on the operational voltage range\u003csup\u003e39\u003c/sup\u003e.To investigate the cyclic stability and switching time of ECDs, we measured the transmittance change at a given wavelength. The switching time is defined as the time taken for the transmittance to reach 90% of its full change after the application of voltage.\u0026nbsp;\u003c/p\u003e\n\u003cp\u003eAs depicted in Figure 4 (a), the optical contrast of P2-a is 30% and it maintains 99% even after switching for 2535718 s (126786 cycles). As shown in Figure 5(a), it requires 1.9 s of coloring and 1.9 s of bleaching. As shown in Figure 4 (b), the P1-b device remains extremely stable even after as many as 58735 s (2936 cycles). As presented in Figure 5(b), its coloring time is 0.95 s and the bleaching time is also 0.98 s. As shown in Figure 4(c), the P2-c device remained stable after 191713 s (9585 cycles) and the coloring time is 0.82 s and the bleaching time is 0.86 s (Figure5(c)). As shown in Figure 4(d), after 194812s (9740 cycles), the cyclic stability of P2-d fluctuates only slightly. Figure 5 (d) illustrates that the coloring time is 0.93 s and the bleaching time is 0.96 s. Figure 4 (e) shows the cyclic stability of the device after 101153 s (5075 cycles) and its coloring time is 0.93 s and a beaching time is 0.96 s (Figure 5e). As shown in Figure 4(f), the P2-f device, after 51411 s (2570 cycles), exhibits a slight decline in cyclic stability. Its coloring time is 3.75 s, and its bleaching time is 3.66 s.\u0026nbsp;\u003c/p\u003e\n\u003cp\u003eFast switching time is attributed to the fact that copolymerization extends conjugation, thereby allowing \u0026pi;-electrons to travel more freely across the molecule\u003csup\u003e40\u003c/sup\u003e. This improves charge transport and enables a quicker response to electric fields, ultimately shortening the response times. In the quest for sustained long-term cyclic stability, it is imperative not only to constrain the low operational voltage range but also to meticulously uphold a dynamic equilibrium between electrons and ions at the active electrode interface during the redox process\u003csup\u003e41\u003c/sup\u003e. These devices exhibit outstanding cyclic stability and fast switching times, demonstrating that the P2 series polymers have excellent performance. This series of data fully demonstrates the high performance of these devices. To demonstrate the scalability of the device, a large-area ECD 100 cm\u0026sup2; was fabricated, showcasing its potential for widespread application and facilitating its path towards industrialization (see Video 1). Generally, the darker the copolymer, the more difficult it is to switch to being transmissive. Its minimum transmittance is below 2%, and the contrast is about 30%, making it ideal materials for manufacturing smart automotive sunroofs (Figure 2b).\u003c/p\u003e\n\u003cp\u003eTo investigate further evaluate the colorimetric properties of different devices, we measured the color coordinates of each device in neutral and summarized the results as Table 2.\u0026nbsp;P2-a demonstrates a notably dark hue with an L* value of 10.57, suggesting minimal lightness, and the color tends toward the red and blue regions, with a* and b* values of 10.53 and -14.93, respectively. This is consistent with the visible absorption spectrum of P2-a, as the polymer transmits a small amount of red light and slightly more blue light. P2-b, with an L* value of 19.17, is relatively darker yet exhibits nearly neutral a* and b* values, suggesting it\u0026apos;s close to black.\u0026nbsp;P2-c, with an L* value of 40.84, is one of the lighter shades and it looks mostly green and blue, because its a* and b* values are more on the negative side. P2-d is characterized by a medium lightness level with an L* value of 33.76 and exhibits green and blue tendencies with a* and b* values of -17.24 and -16.34, respectively. P2-e and P2-f, with L* values of 12.92 and 40.84, respectively, with greenish-blue chromaticity, aligning with their negative a* and b* values. They primarily appear black with slight hints of blue and green, which is consistent with their absorption curves showing lower absorption rates in the blue and green light regions.\u003c/p\u003e\n\u003cp\u003e\u0026nbsp;Table 2. L*a*b* values in neutral state of P2 ECDs\u003c/p\u003e\n\u003ctable border=\"1\" cellspacing=\"0\" cellpadding=\"0\" width=\"661\"\u003e\n \u003ctbody\u003e\n \u003ctr\u003e\n \u003ctd width=\"4.833836858006042%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"16.61631419939577%\" colspan=\"2\" valign=\"top\"\u003e\n \u003cp\u003eP2-a\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"15.709969788519638%\" colspan=\"2\" valign=\"top\"\u003e\n \u003cp\u003eP2-b\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"15.709969788519638%\" colspan=\"2\" valign=\"top\"\u003e\n \u003cp\u003eP2-c\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"15.709969788519638%\" colspan=\"2\" valign=\"top\"\u003e\n \u003cp\u003eP2-d\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"15.709969788519638%\" colspan=\"2\" valign=\"top\"\u003e\n \u003cp\u003eP2-e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"15.709969788519638%\" colspan=\"2\" valign=\"top\"\u003e\n \u003cp\u003eP2-f\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd width=\"4.833836858006042%\" valign=\"top\"\u003e\n \u003cp\u003eL\u003csup\u003e*\u003c/sup\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.006042296072508%\" valign=\"top\"\u003e\n \u003cp\u003e10.57\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e19.17\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e15.95\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e33.76\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e12.92\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e40.84\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd width=\"4.833836858006042%\" valign=\"top\"\u003e\n \u003cp\u003ea\u003csup\u003e*\u003c/sup\u003e\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.006042296072508%\" valign=\"top\"\u003e\n \u003cp\u003e10.53\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e0.78\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-10.95\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-17.2\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-13.35\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-17.44\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd width=\"4.833836858006042%\" valign=\"top\"\u003e\n \u003cp\u003eb*\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.006042296072508%\" valign=\"top\"\u003e\n \u003cp\u003e-14.93\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-0.35\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-14.44\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-16.34\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-16.70\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"7.099697885196375%\" valign=\"top\"\u003e\n \u003cp\u003e-29.71\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd width=\"8.610271903323262%\" valign=\"top\"\u003e\n \u003cp\u003e\u0026nbsp;\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003c/tbody\u003e\n\u003c/table\u003e"},{"header":"Conclusion","content":"\u003cp\u003eIn this contribution, precise control of the absorption spectra of conjugated polymers was achieved by simply adjusting the feed ratios of four types of monomers in a random direct C\u0026ndash;H arylation polymerization. We present the most broadly absorbing black-to-transmissive switching conjugated EC polymers, realized through the strategic selection of four functional monomers. A novel strategy has been implemented to enhance the performance of ECDs by synergistically improving the ionic conductivity of copolymers. The ECDs exhibit excellent overall performance, marked by high reversibility (\u0026ge;\u0026thinsp;126,786 cycles), superior coloration efficiency (\u0026ge;\u0026thinsp;1,273 cm\u003csup\u003e2\u003c/sup\u003e/C), and rapid switching times (0.82 s for coloring and 0.86 s for bleaching), suggesting that these copolymers possess exceptional properties. Performance comparisons with similar materials are detailed in Table\u0026nbsp;\u003cspan refid=\"Tab3\" class=\"InternalRef\"\u003e3\u003c/span\u003e. This study not only highlights advancements in the design of high-performance black EC materials but also provides significant inspiration for other applications, such as organic photovoltaics and sensor technology.\u003c/p\u003e \u003cp\u003e \u003cdiv class=\"gridtable\"\u003e\u003ctable float=\"Yes\" id=\"Tab3\" border=\"1\"\u003e \u003ccaption language=\"En\"\u003e \u003cdiv class=\"CaptionNumber\"\u003eTable 3\u003c/div\u003e \u003cdiv class=\"CaptionContent\"\u003e \u003cp\u003ePerformance of ECDs compared to other similar work\u003c/p\u003e \u003c/div\u003e \u003c/caption\u003e \u003ccolgroup cols=\"7\"\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c1\" colnum=\"1\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c2\" colnum=\"2\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c3\" colnum=\"3\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c4\" colnum=\"4\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c5\" colnum=\"5\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c6\" colnum=\"6\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c7\" colnum=\"7\"\u003e\u003c/div\u003e \u003cthead\u003e \u003ctr\u003e \u003cth align=\"left\" colname=\"c1\"\u003e \u003cp\u003eNumber\u003c/p\u003e \u003c/th\u003e \u003cth align=\"left\" colname=\"c2\"\u003e \u003cp\u003eColor in the ox/red state\u003c/p\u003e \u003c/th\u003e \u003cth align=\"left\" colname=\"c3\"\u003e \u003cp\u003eAbsorption range (nm)\u003c/p\u003e \u003c/th\u003e \u003cth align=\"left\" colname=\"c4\"\u003e \u003cp\u003eVoltage range (V/V)\u003c/p\u003e \u003c/th\u003e \u003cth align=\"left\" colname=\"c5\"\u003e \u003cp\u003eCE (cm\u003csup\u003e2\u003c/sup\u003e/C)\u003c/p\u003e \u003c/th\u003e \u003cth align=\"left\" colname=\"c6\"\u003e \u003cp\u003eCyclic stability\u003c/p\u003e \u003cp\u003e(cycles)\u003c/p\u003e \u003c/th\u003e \u003cth align=\"left\" colname=\"c7\"\u003e\u0026nbsp;\u003c/th\u003e \u003c/tr\u003e \u003c/thead\u003e \u003ctbody\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e1\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e500\u0026ndash;700 nm\u003c/p\u003e \u003cp\u003e350nm -450 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e-0.6 / 0.7 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e10000\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef \u003csup\u003e5\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e2\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eGreen to transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e300\u0026ndash;410 nm\u003c/p\u003e \u003cp\u003e450nm-620 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e-0.4 / 0.85 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e10000 (loss 5%)\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e42\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e2\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlue-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e380\u0026ndash;420 nm\u003c/p\u003e \u003cp\u003e500\u0026ndash;740 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e-0.4 / 0.96 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e10000 (loss 7%)\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e43\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e4\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlue-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e420\u0026ndash;710 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e-1 / 1 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e\u0026nbsp;\u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e11\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e5\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e400\u0026ndash;700 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e\u0026minus; 0.6 / 1.5 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e18000 (loss 8%)\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e6\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e6\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e450\u0026ndash;750 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e-0.6 / 1.6 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e500\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e4\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e7\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e380\u0026ndash;430 nm\u003c/p\u003e \u003cp\u003e450\u0026thinsp;\u0026minus;\u0026thinsp;760 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e-0.2 / 0.7 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e360\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e29\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e8\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e450\u0026ndash;600 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e-2 / 2 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e28\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e9\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e400\u0026ndash;700 nm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e-0.3 / 0.8 V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e333\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e31\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e \u003cp\u003e10\u003c/p\u003e \u003cp\u003e11\u003c/p\u003e \u003cp\u003e12\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003cp\u003eBlack-to-transmissive\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e400\u0026ndash;470 nm\u003c/p\u003e \u003cp\u003e550\u0026ndash;750 nm\u003c/p\u003e \u003cp\u003e-\u003c/p\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e1.6 / -1.6 V\u003c/p\u003e \u003cp\u003e-0.6/ 0.8V\u003c/p\u003e \u003cp\u003e-2.5/ 0V\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e-\u003c/p\u003e \u003cp\u003e-\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e-\u003c/p\u003e \u003cp\u003e1000\u003c/p\u003e \u003cp\u003e4000\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003eRef\u003csup\u003e8\u003c/sup\u003e\u003c/p\u003e \u003cp\u003eRef\u003csup\u003e44\u003c/sup\u003e\u003c/p\u003e \u003cp\u003eRef\u003csup\u003e45\u003c/sup\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\"\u003e\u0026nbsp;\u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003e\u003cb\u003eBlack-to-transmissive\u003c/b\u003e\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e\u003cb\u003e320\u0026ndash;760 nm\u003c/b\u003e\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e \u003cp\u003e\u003cb\u003e-0.1 /0.8 V\u003c/b\u003e\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003e\u003cb\u003e1273\u003c/b\u003e\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e\u003cb\u003e126786 (loss 1%)\u003c/b\u003e\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c7\"\u003e \u003cp\u003e\u003cb\u003eThis work\u003c/b\u003e\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003c/tbody\u003e \u003c/colgroup\u003e \u003c/table\u003e\u003c/div\u003e \u003c/p\u003e"},{"header":"Declarations","content":"\u003cp\u003e\u003cstrong\u003eData availability\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe data used in this study are available from the corresponding author on reasonable request.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eCompeting interests\u003c/strong\u003e\u0026nbsp;\u003c/p\u003e\n\u003cp\u003eThe authors declare no competing interests.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eAcknowledges\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThis work is financially supported by Shenzhen Fundamental Research Program (No. GXWD20201231165807007-2020081011134000), Shenzhen Science and Technology Program (JSGG20220831094202004), NSFC (22275003). It also is supported by China Scholarship Council (No.202306290018, Recipient: Chen Dinghui).\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eAuthor contributions\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eH.M. and W.H. conceived the project. D.C. and Q.R. performed material synthesis, structural characterization, devices fabrication, and electrochromic measurements. D.C. also collaborated with T.Z. in synthesizing the material.\u0026nbsp;Moreover, D.C., Q.R., and Z.T. designed the experiments. D.C. and H.M.\u0026nbsp;wrote\u0026nbsp;the manuscript with contributions from all authors during the review and editing process.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eCorrespondence and requests for materials\u003c/strong\u003e should be addressed to Hong Meng.\u003c/p\u003e"},{"header":"References","content":"\u003col\u003e\n\u003cli\u003eGu CJ, A. B.Zhang, Y. M.Zhang, S. X. 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DArP is an environment friendly polymerization for the donor\u0026ndash;acceptor (D\u0026ndash;A) type\u003csup\u003e46\u003c/sup\u003e. The molecular weights of polymers are provided in Table 1.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eMaterials\u0026nbsp;\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eTri(ethylene glycol) monoethyl ether, ethyl 2-hydroxybenzoate, 2,2-bis(bromomethyl)-1,3-propanediol,\u0026nbsp;Potassium carbonate (K\u003csub\u003e2\u003c/sub\u003eCO\u003csub\u003e3\u003c/sub\u003e), chloroform, Pd(OAC)\u003csub\u003e2\u003c/sub\u003e, PiVOH,\u0026nbsp;tri(ethylene glycol) monoethyl ether were purchased from Bide. Tetrahydrofuran (THF), ethanol, methanol, N,N-dimethylformamide (DMF), N,N-dimethylacetamide (DMAc) were bought from Aladdin. 2-dibromo-9-fluorenone, 4-toluene sulfonyl chloride, methanesulfonic acid purchased from Energy-chemical. Indium tin oxide (ITO)\u0026nbsp;glasses\u0026nbsp;were purchased from south China Xiangcheng Technology Co., LTD.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eMeasurements\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe 1H NMR and 13C NMR spectra were recorded in CDCl\u003csub\u003e3\u0026nbsp;\u003c/sub\u003esolution at room temperature using Bruker AVANCE 500 (or 400) NMR spectrometers. Absorption spectra were obtained using a PerkinElmer Lambda 750 spectrophotometer. Cyclic Voltammetry (CV) curves were generated using a Gamry 1000B electrochemical workstation. For potential-dependent in-situ absorption measurements, the Gamry 1000B workstation was used in conjunction with the PerkinElmer Lambda 750 spectrophotometer. Thermal gravimetric analysis (TGA) was performed under a nitrogen (N\u003csub\u003e2\u003c/sub\u003e) atmosphere from 30 to 800 \u0026deg;C at a heating rate of 10 \u0026deg;C/min using a Mettler Toledo TGA2 instrument. Average molecular weights and polydispersity indices (PDIs) were determined using gel permeation chromatography (Waters ACQUITY Advanced Polymer Chromatograph).\u0026nbsp;L*a*b* values were based on the International Commission\u0026apos;s 1931 L*a*b* color model.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eFabrication of devices\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe working electrode was prepared by bar coating method, and 40 mg/mL polymer solution was coated on indium tin oxide (ITO) substrate with a size of 3 \u0026times; 3 cm. The counter electrode was prepared by bar coating 15 mg/mL PB solutionon the ITO substrate. Before device fabrication, ITO coated with polymer or PB was vacuum-dried at 60 \u0026deg;C for half an hour. The solid-state electrolyte was uniformly dispersed on the surface of the polymer film. Subsequently, ITO coated with PB was pressed onto working electrode. The device is then cured using ultraviolet light for 10 seconds to bond the working electrode and the counter electrode together. Subsequently, the device was encapsulated using UV and thermosetting OLED adhesive. Finally, it was cured with ultraviolet light for 20 seconds, followed by vacuum drying at 80 ℃ for 50 minutes.\u003c/p\u003e"}],"fulltextSource":"","fullText":"","funders":[],"hasAdminPriorityOnWorkflow":false,"hasManuscriptDocX":true,"hasOptedInToPreprint":true,"hasPassedJournalQc":"","hasAnyPriority":true,"hideJournal":false,"highlight":"","institution":"","isAcceptedByJournal":true,"isAuthorSuppliedPdf":false,"isDeskRejected":"","isHiddenFromSearch":false,"isInQc":false,"isInWorkflow":false,"isPdf":false,"isPdfUpToDate":true,"isWithdrawnOrRetracted":false,"journal":{"display":true,"email":"[email protected]","identity":"nature-portfolio","isNatureJournal":true,"hasQc":false,"allowDirectSubmit":false,"externalIdentity":"","sideBox":"","snPcode":"","submissionUrl":"","title":"Nature Portfolio","twitterHandle":"","acdcEnabled":false,"dfaEnabled":false,"editorialSystem":"ejp","reportingPortfolio":"","inReviewEnabled":true,"inReviewRevisionsEnabled":false},"keywords":" organic optoelectronics, black electrochromic materials, transparent, high stability, coloration efficiency","lastPublishedDoi":"10.21203/rs.3.rs-3939829/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-3939829/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"\u003cp\u003eThe black-to-transparent electrochromism is hailed as the \"Holy Grail\" of organic optoelectronics. However, designing black electrochromic (EC) materials that fully absorb in the visible light region remains challenging. Electroactive materials that simultaneously possess excellent cyclic stability, fast switching times, and high coloration efficiency are extremely rare. In this work, copolymers capable of fully absorbing across the entire visible spectrum have been successfully designed through judicious selection of four types of monomers. We introduce two types of polar side chains, which synergistically improve the ionic conductivity of copolymer, thereby enhancing the performance of electrochromic devices(ECDs). ECDs exhibit unprecedentedlong-term cyclic stability, surpassing all previously reported high cyclic stability devices with over 126,786 cycles. Additionally, they achieve a coloration efficiency of 1273 cm²/C, which exceeds that of every high coloration efficiency ECDs present so far, along with fast coloring/bleaching times of 0.82 s/0.86 s. This study presents a new strategy for the design and synthesis of high-performance black electrochromic copolymers.\u003c/p\u003e","manuscriptTitle":"Unlocking the Full Spectrum: A Paradigm Shift in Electrochromic Devices with High-Performance Black Conjugated Polymers","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2024-02-23 06:22:51","doi":"10.21203/rs.3.rs-3939829/v1","editorialEvents":[],"status":"published","journal":{"display":true,"email":"[email protected]","identity":"nature-communications","isNatureJournal":true,"hasQc":false,"allowDirectSubmit":false,"externalIdentity":"NCOMMS","sideBox":"Learn more about [Nature Communications](http://www.nature.com/ncomms/)","snPcode":"","submissionUrl":"https://mts-ncomms.nature.com/","title":"Nature Communications","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"ejp","reportingPortfolio":"Nature Communications","inReviewEnabled":true,"inReviewRevisionsEnabled":false}}],"origin":"","ownerIdentity":"9e51a984-f0e0-4267-9005-9d09daf79061","owner":[],"postedDate":"February 23rd, 2024","published":true,"recentEditorialEvents":[],"rejectedJournal":[],"revision":"","amendment":"","status":"published-in-journal","subjectAreas":[{"id":28907141,"name":"Physical sciences/Materials science/Materials for devices/Electronic devices"},{"id":28907142,"name":"Physical sciences/Materials science/Materials for optics"}],"tags":[],"updatedAt":"2024-10-01T07:05:51+00:00","versionOfRecord":{"articleIdentity":"rs-3939829","link":"https://doi.org/10.1038/s41467-024-52430-2","journal":{"identity":"nature-communications","isVorOnly":false,"title":"Nature Communications"},"publishedOn":"2024-09-30 04:00:00","publishedOnDateReadable":"September 30th, 2024"},"versionCreatedAt":"2024-02-23 06:22:51","video":"","vorDoi":"10.1038/s41467-024-52430-2","vorDoiUrl":"https://doi.org/10.1038/s41467-024-52430-2","workflowStages":[]},"version":"v1","identity":"rs-3939829","journalConfig":"researchsquare"},"__N_SSP":true},"page":"/article/[identity]/[[...version]]","query":{"redirect":"/article/rs-3939829","identity":"rs-3939829","version":["v1"]},"buildId":"qtupq5eGEP_6zYnWcrvyt","isFallback":false,"isExperimentalCompile":false,"dynamicIds":[84888],"gssp":true,"scriptLoader":[]}