Diblock copolymers consisting of electron-donating poly[2,7-(9,9-dihexylfluorene)] (PF) rods and electron-withdrawing poly(pendent isoindigo) (Piso) coils were designed and synthesized through a click reaction. The electronic properties and interchain organization of the copolymers could be tuned by varying the PF/Piso ratio (PF14-b-Pison (n=10, 20, 60 and 100)). The highest occupied molecular orbital and lowest unoccupied molecular orbital energy levels of the studied polymers were progressively reduced as the length of Piso increased, affecting the charge trapping and intramolecular charge transfer environment between PF and Piso domains. Thermally treated PF14-b-Pison thin films exhibited a clear nanofibrillar structure, and the d-spacing was enhanced systematically as the Piso chain length increased. Resistive memory characteristics were explored with a sandwich indium tin oxide/PF14-b-Pisons/Al device configuration. The enhanced conjugated PF conducting channels led to stable resistance switching behavior, exhibiting volatile SRAM (static random access memory) (PF14-b-Piso10) and nonvolatile WORM (write-once-read-many-times) (PF14-b-Piso20, PF14-b-Piso60, PF14-b-Piso100) characteristics with a large ON/OFF ratio (106) and a stable retention time (104 s). A more appealing feature is that such memory cells were integrated on a soft poly(dimethylsiloxane) substrate, allowing for the development of a stretchable data storage device. Reliable and reproducible electrical characteristics, including SRAM- and WORM-type memories, could be explored as the device was stretched under an applied tensile strain ranging from 0 to 50%. The studied donor–acceptor copolymers indeed showed great potential for stretchable electronic applications with controllable digital information storage characteristics.
Polymer-based electrical bistable memory devices have been extensively studied owing to their advantages of structural flexibility, low-cost, printability and three-dimensional stacking.1, 2, 3 Such memories can be switched between high and low resistance states (that is, OFF and ON states) by applying an external electric field.4, 5, 6, 7, 8, 9, 10, 11, 12 Electrical memory characteristics can generally be divided into two categories, namely nonvolatile (for example, WORM (write-once-read-many-times) and flash) and volatile memory (for example, dynamic random access memory and SRAM (static random access memory)), which show different tendencies for the stored charges to dispel. The volatility of these digital information storage devices can be controlled by (1) the charge transfer or charge trapping ability of the active materials and (2) the morphological packing structures in the memory layers. Conjugated block copolymers can effectively manipulate charge storage volatility because of their unique self-organization properties, on the basis of the chemical structures of different block segments.3 Conjugated rod-coil copolymers have attracted extensive research interest for electronic applications because the conjugated rods typically possess strong interchain π–π interactions to facilitate conducting channels, whereas the soft coil blocks provide the degree of freedom for polymer chain movement to induce self-assembled molecular packing.6
Polyfluorene (PF) is a well-known conjugated moiety for optoelectronics (for example, light-emitting diodes,13 field-effect transistors,14 and memory devices15, 16, 17) owing to its good electron-donating ability, efficient hole carrier transport and outstanding thermal stability. PF-based rod-coil block copolymers have been explored for resistive memory applications. A volatile SRAM PF-b-Poly(2-vinylpyridine) memory with tunable charge storage duration was previously reported. Moreover, an electron-withdrawing [6,6]-phenyl-C61-butyric acid methyl ester was added to associate the donor–acceptor (D–A) charge transfer interaction, converting the memory from volatile SRAM to nonvolatile WORM behavior.16 Such a D–A effect, however, must be generated using a polymer composite (that is, adding an extra functional molecule), which may face the bottlenecks of thin-film uniformity and device reproducibility. The development of conjugated rod-coil block copolymers with both donor and acceptor segments that would allow for control over the charge transfer interaction, charge carrier transport and thin-film morphology at the same time would provide significant advantages.
Organic stretchable electronics, on the other hand, have developed rapidly in recent years and possess the potential to be biocompatible with wearable devices, electronic skins and health-care monitors.18, 19, 20, 21, 22 In the field of resistive memories, flexible and twistable devices have already been reported to exhibit stable memory functionality under deformation,4, 17, 23, 24 but research on stretchable devices is still relatively rare, limited by the ductility of active materials. Chen and his coworkers evaluated a stretchable memory device using a poly(3-butylthiophene)/poly(methyl methacrylate) blending film on a pre-strained poly(dimethylsiloxane) (PDMS) substrate. Reliable resistive switching behavior and strong data retention ability were obtained as the devices were stretched by up to 50%.22 Note that the uniformity of the active layer of such stretchable devices may also be limited because two types of polymers are required and could reduce the yield of memory cells in a device. However, stretchable memory devices using donor–acceptor copolymer systems have not yet been developed to the best of our knowledge. The fabrication of a stretchable memory with a single active layer component with good thin-film ductility and tunable electrical properties, therefore, is essential for developing future high-performance data storage electronics.
In this study, we developed a series of rod-coil diblock copolymers, PF14-b-Pisons, containing poly[2,7-(9,9-dihexylfluorene)] (PF) electron-donating rods with electron-withdrawing poly(pendent isoindigo) (Piso) coils. The PF and Piso blocks were synthesized through chain-growth Suzuki–Miyaura coupling polymerization25, 26 and atom transfer radical polymerization methods,27, 28 respectively, and the target diblock copolymers were obtained via a click coupling reaction (Scheme 1). The thermal, optical and electrochemical characteristics of the studied block copolymers were explored systematically. In addition, the morphology of the prepared PF14-b-Pisons thin films was investigated using atomic force microscopy (AFM) and grazing-incidence small-angle X-ray scattering (GISAXS). The resistive switching behaviors were probed, and the charge carrier storage volatility was correlated with the PF/Piso block ratio and the self-assembled nanostructures. One appealing feature is that stretchable memory devices were fabricated by integrating the studied block copolymers on a soft PDMS substrate with a high ON/OFF ratio of 105 under 0–50% applied tensile strain. The studied block copolymers indeed allow for the combination of conjugated rods for superior electrical properties and soft coils for enhanced material ductility, leading to a polymer active layer that possesses good digital information storage characteristics and thin-film stretchability for wearable electronic applications.
Materials and methods
Fabrication of stretchable memory devices
A PDMS (Sylgard 184, Dow Corning, Midland, MI, USA) substrate (~2 mm thick) was prepared at a ratio of 20:1 (base:crosslinker, w/w) and cured for 12 h at 120 °C, and was used to transfer a carbon nanotube (CNT) bottom electrode. CNTs was first spray-coated onto an octadecyltrimethoxysilane-modified Si wafer, and electrode lines were aligned by a shadow mask. Subsequently, the CNT electrodes were transferred onto a PDMS substrate (2 cm × 4 cm) and clamped on a glass side. The CNT/PDMS substrate was then stretched to 50% strain. Next, thermally annealed (100 °C under a nitrogen atmosphere for 2 h) PF14-b-Pison thin films (using the same procedure used to produce memory devices on indium tin oxide (ITO) substrates (Supplementary Information) but prepared on an octadecyltrimethoxysilane-modified Si wafer) were directly transferred onto the pre-strained CNT/PDMS substrate. Finally, Al top electrodes (40 nm thick; perpendicular to the bottom CNT electrode) were deposited using a thermal evaporator at a pressure of 10−6 torr at a deposition rate of 1 Å s−1 and aligned by a regular shadow mask. The prepared stretchable memory devices were released back to the non-stretching condition (that is, 0% strain) before testing.
Results and discussion
The synthetic route for producing the target rod-coil diblock copolymers, poly[2,7-(9,9-dihexylfluorene)]-block-poly(pendent isoindigo) (PF14-b-Pison) is illustrated in Scheme 1. The detailed synthetic parameters are summarized in Table 1 and the Supplementary Information. In accordance with our previous report,29 the ethynyl end-functionalized PF (2, PF14) was prepared with an estimated molecular weight (Mn(NMR)) of 4900 g mol−1 (that is, 14 fluorene repeating units). The azido-terminated Piso (4a–d, N3-Pison (n=10, 20, 60 and 100, respectively)) coils, on the other hand, were synthesized with various lengths.30 The rod-coil diblock copolymers, PF14-b-Pisons (5a–d), were synthesized through the Cu-catalyzed azido-alkyne click reaction of PF14 and N3-Pisons, and Fourier transform infrared spectroscopy was employed to determine whether the reaction was completed (Supplementary Figure S2). Four polymers with different coil lengths were successfully produced, and their polymer properties are listed in Table 1. Figure 1a shows the 1H-NMR (nuclear magnetic resonance) spectrum of PF14-b-Piso20; proton signals originating from the Piso coils (peaks a, c, d, e, h, i and j) and PF moiety (peaks b and l) are clearly observed. A signal attributable to the methylene adjacent to the triazole ring (–N=N–N–CH2–), moreover, was observed at 4.24 p.p.m., suggesting that a link between the PF and Piso blocks was formed. The 1H-NMR signals for the other studied block copolymers were also fitted to our proposed chemical structures (Supplementary Figure S2a). In addition, the results of elemental analyses, including analyses of carbon, hydrogen and nitrogen content, of the PF14-b-Pisons are in good agreement with the theoretical content.
The PF14-b-Piso20 Fourier transform infrared spectroscopy spectrum shows that the characteristic absorption of the azido group at 2098 cm−1 completely disappeared (Figure 1b) because the N3-Piso20 and the ethynyl end-functional PF were fully reacted in the click reaction system.
The size exclusion chromatography (SEC) traces of N3-Pisons and PF14-b-Pisons are depicted in Figure 1c and Supplementary Figure S2c. The elution peak of PF14-b-Pisons shifted to the higher molecular weight region after the click reaction compared with that of N3-Pison, leading to a number-averaged molecular weights (Mn(SEC)) in the range of 9500–58 600 g mol−1 depending on the controllable Piso length. The results of 1H-NMR, Fourier transform infrared spectroscopy, SEC and elemental analysis suggest that well-defined PF14-b-Pisons with Piso coil lengths of 10, 20, 60 and 100 repeating units were effectively produced through the click reaction between PF14 and N3-Pisons. All the studied block copolymers are well soluble in common organic solvents, such as chloroform, tetrahydrofuran and toluene.
Thermogravimetric analysis and differential scanning calorimetry were used to detect the thermal properties of PF14, N3-Piso100 and PF14-b-Pison, as illustrated in Supplementary Figure S3 and summarized in Table 1. The thermal decomposition temperatures (Td, 5% weight-loss) of PF14 and N3-Piso100 are 400 and 277 °C, respectively. The Td values of the PF14-b-Pisons are located between those associated with the decomposition of the PF and Piso segments. Although the thermal degradation of these block copolymers could occur at two distinct Td temperatures, the narrow temperature ranges of the two blocks make them indistinguishable. On the basis of differential scanning calorimetry heating traces, on the other hand, the studied PF14-b-Pisons exhibit a broad transition temperature, with the glass transition temperatures (Tg) ranging from 73.7 to 83.8 °C, which are between the Tg of the parent PF (69.3 °C) and Piso (87.1 °C) blocks. Similarly, we observed only one broad thermal transition on the prepared block copolymers instead of two distinct Tg values, which was also caused by the similar Tg values of PF (69.3 °C) and Piso (87.1 °C). Thus, the observation of only one transition temperature in the studied block copolymers does not mean that there is no microphase separation.
Ultraviolet–visible absorption spectra of the synthesized polymer films of PF14, Piso100 and PF14-b-Pisons are shown in Figure 2a. Their corresponding maximum absorption wavelengths (λmax) and optical band gaps (Egopt), in addition, are summarized in Table 2. PF14 clearly exhibits a λmax at 371 nm, whereas the Piso homopolymer (that is, Piso100) shows two spin allowed π–π* transitions at 276 and 337 nm. All the PF14-b-Pison-based thin films possessed two distinct signals: (1) a narrow peak at ~276 nm, attributed to the absorption of Piso coils, the intensity of which increased with the content of Piso; (2) a broad absorption peak over the range of 350–373 nm, which was affected by both the PF and Piso moieties, and the intensity of which decreased distinctively with the blue shift in λmax from 373 to 350 nm as the content of the Piso segment increased. The optical band gaps (Egopt) of PF14 and Piso100 estimated from the onset of solid-state absorption are 2.79 and 3.28 eV, respectively. Indeed, the series of rod-coil copolymers, PF14-b-Pisons, showed Egopt values between those of their parent building blocks (that is, PF and Piso) of 2.84 (PF14-b-Piso10), 2.98 (PF14-b-Piso20), 3.00 (PF14-b-Piso60) and 3.06 (PF14-b-Piso100) eV. It should be noted that the Egopt values of the studied block copolymers became slightly larger owing to the increased Piso content, indicating that the PF/Piso coil-to-rod ratio can significantly affect their optoelectronic properties.
Furthermore, the solid-state photoluminescence (PL) spectra (Supplementary Figure S4) were characterized to clarify the strength of the intermolecular interaction between the electron-donating PF (donor) and electron-withdrawing Piso (acceptor) in the studied block copolymer. PF14 exhibited the strongest photoluminescence emission, and possessed two distinct peaks located at 420 and 445 nm, which are commonly observed among conjugated poly(fluorene)s. As the content of the Piso acceptor was increased, the photoluminescence emission was remarkably quenched owing to the donor–acceptor interaction, indicating charge transfer in the PF14-b-Pison thin films.31
The electrochemical properties of the studied block copolymers were investigated by cyclic voltammetry to understand the relationship between chemical structures and energy levels, as depicted in Figure 2b and summarized in Table 2. The highest occupied molecular orbital (HOMO) energy levels were calculated from the onset of oxidation waves in the cyclic voltammetry curves with reference to ferrocene (4.8 eV), whereas the lowest unoccupied molecular orbital (LUMO) energy levels were estimated from the difference between the optical band gap and HOMO level. The HOMO levels obtained for PF14, PF14-b-Piso10, PF14-b-Piso20, PF14-b-Piso60, PF14-b-Piso100 and Piso100 were −5.48, −5.55, −5.74, −5.84, −6.06 and −6.24 eV, respectively, and their corresponding LUMO levels were −2.69, −2.71, −2.76, −2.84, −3.00 and −2.96 eV, respectively. Both the HOMO and LUMO energy levels of PF14-b-Pison were systematically reduced with increasing Piso length, as illustrated in Figure 2c. The HOMO energy level of PF14-b-Pison was affected by both the electron-donating PF and electron-withdrawing Piso blocks. The intrachain or interchain charge transfer of PF and Piso in the block copolymers led to a decrease in the HOMO energy level with increasing Piso chain length. It should be noted that the microphase separation of the two blocks could prevent intrachain charge transfer, and thus interchain charge transfer would be significant in the case of thin films, leading to a change in the HOMO level with increasing Piso block length.
Nanostructures on PF14-b-Pison thin-film surfaces were investigated using AFM. For the as-cast polymer films (that is, without thermal annealing treatment), no distinct surface structure was observed for any of the studied block copolymers (Supplementary Figure S5). The thermally treated PF14-b-Pison thin films, however, presented a distinct nanofibrillar structure on the surface (Figure 3). Short and rod-like aggregates were observed on the surface of PF14-b-Piso10 films (Figure 3a) owing to the strong π–π interaction of the PF-conjugated segments. As the content of Piso coils was increased, more interestingly, a fibrillar structure was clearly observed (Figure 3b–d). This structure is attributed to the molecular packing of conjugated PF domains, and the size and density of these nanofibers could be controlled by tuning the PF/Piso block ratio. The driving force for creating these self-assembly morphologies on our block copolymer surfaces is the π-electron interaction between the conjugated PF rods and the nonconjugated soft chains (Piso). The nanofibrillar PF-aggregated domains, hence, can be formed owing to a balance between the thermodynamics and kinetics of crystalline/amorphous (that is, PF/Piso) domains.
To further investigate the self-assembly behaviors of the PF14-b-Pisons, we examined the thermally annealed PF14-b-Pison thin films using GISAXS. Figure 3e shows the one-dimensional GISAXS profiles of thermally annealed thin films of the studied block copolymers. Thin films prepared from PF14-b-Piso10, PF14-b-Piso20, PF14-b-Piso60 and PF14-b-Piso100 exhibited a clear first-order scattering peak located at q*=0.0374, 0.0302, 0.0257 and 0.0215 Å−1, respectively, and the corresponding d-spacing values (that is, average center-to-center distance of the PF nanostructures), calculated from the scattering formula d=2π/q*, were 16.8, 20.8, 24.4 and 29.2 nm, respectively. The GISAXS results reveal that the d-spacing of PF14-b-Pison increased systematically with the increase in the Piso chain length from 10 to 100 repeating units, which is consistent with the recorded AFM phase images. The abovementioned morphological results demonstrate that the thin films on the basis of the studied PF14-b-Pison block copolymers possess well-defined self-assembled nanostructures after thermal annealing, and these tunable nanofibrillar structures may further influence the electrical characteristics effectively.
Figure 4 and Supplementary Figure S6 show the representative current density–voltage (J–V) characteristics of devices fabricated from PF14, Piso100 and PF14-b-Pisons. The structure–property relationship was probed using a cross bar array-designed two-terminal resistive memory with a device configuration of ITO/PF14-b-Pison/Al. A voltage was applied, with a step of 0.05 V, to the top electrode (Al). Stable electrical switching behavior could be obtained using thermally annealed PF14-b-Pison thin films. The J–V curves of the PF14-b-Piso10-based device (Figure 4a) were initially in a high resistance state (that is, OFF state; ‘0’ signal in data storage) with a current density in the range of 10−9–10−10 A as the voltage was swept from 0 to −1.5 V. Then, the current abruptly switched from a high resistance state to a low resistance state (that is, ON state; ‘1’ signal in data storage) with a threshold voltage of approximately −1.5 V. It should be noted that this electronic transition from the OFF state to the ON state during the scanning serves as the writing process. The PF14-b-Piso10 memory can be kept in the ON state using a subsequent sweep from 0 to −4.0 V after writing (sweep 2), showing bistable conductance states with an ON/OFF current ratio of up to 104. A third sweep was conducted using the same memory cell after turning off the power for ~5 min, and the device could be reprogrammed from the OFF state to the ON state once again with a turn-on voltage of −1.5 V. We therefore investigated the device under repeating writing/relaxation cycles, observing that the device could be maintained in the ON state for a period of 5–10 min after the removal of the power supply and then gradually switched back to the OFF state, indicating that the PF14-b-Piso10-based memory device exhibits volatile SRAM behavior.
The J–V curves of PF14-b-Piso20-, PF14-b-Piso60-and PF14-b-Piso100-based memory devices, on the other hand, illustrated similar electrical switching characteristics through five voltage sequences (Figure 4b–d): 0 to −4 V (sweep 1); 0 to −4 V (sweeps 2 and 4); and 0 to 4 V (sweeps 3 and 5). The memory cell was initially in the high-resistance OFF state and then switched to the low-resistance ON state at the appropriate threshold voltage. The current level was then maintained in the ON state for the subsequent negative or positive sweeps (sweeps 2 and 3) with an ON/OFF current ratio of 105–106 at −1 V. This memory device, moreover, could not return to the OFF state after turning the power off or even applying a reverse bias (sweeps 4 and 5), suggesting nonvolatile WORM memory characteristics.
The abovementioned results suggest that electrical switching properties are strongly dependent on the PF/Piso ratio in the block copolymers. The conjugated PF rods (that is, PF14) possess a relatively high p-channel charge carrier mobility and show conductor characteristics without any changes in resistance state (Supplementary Figure S6a). However, only highly resistant insulating behavior was obtained for the pendent electron-withdrawing isoindigo coils (that is, Piso100) owing to their nonconjugated backbone (Supplementary Figure S6b). Thus, resistive memory switching was induced from the PF conducting channels in an insulating Piso matrix, leading to tunable charge storage volatility by manipulating the PF/Piso block ratio and controlling the surface structure of PF14-b-Pisons.
The memory characteristics of the PF14-b-Pisons-based as-cast thin films (that is, without thermal annealing) were also addressed to clarify the effects of the thermal annealing treatment and nanostructured morphologies on the resistive switching behavior (Supplementary Figure S7). The memory characteristics of the studied polymers were generally similar (SRAM (PF14-b-Piso10) or WORM (PF14-b-Piso20 and PF14-b-Piso60)) to those of the active thin film with or without thermal annealing. However, the characteristics were different from those of the PF14-b-Piso100-based device. The as-cast PF14-b-Piso100 memory could not generate any resistance conversion under a voltage bias, whereas the corresponding thermally annealed thin film could exhibit WORM-type characteristics, because conducting channels were formed in the PF nanostructures, as indicated by AFM imaging. Statistics associated with the memory parameters, such as the threshold voltage, ON state current level and ON/OFF ratio, are summarized in Figure 5. The operating deviation of the threshold voltage (Figure 5a and Supplementary Figure S8) was significantly reduced as the studied devices were treated by thermal annealing. The threshold voltage, furthermore, increased with the increasing length of the Piso segments, which was mainly attributed to the content of the PF and Piso blocks. As the content of PF was decreased with increasing Piso length, the effective conducting region was minimized and the charge injection barrier (that is, energy difference between the HOMO level and the work function of the ITO electrode) was increased such that the device required a larger electrical driving force to be switched on. The ON state current level and the ON/OFF current ratio of the studied devices were also investigated statistically (Figure 5b). The ON state current density was significantly enhanced after thermal annealing owing to the nanofibrillar structures as well as the effective conducting channels of the conjugated PF segments. Thus, the current level and, in turn, the ON/OFF current ratio of the memory device were increased. In addition, the value of the ON state current was decreased with the increase in the length of the Piso coils. This trend is also attributed to the relative content of PF and Piso blocks because the charge transport region was diminished as the content of Piso was increased, and thus, a lower ON current response was obtained.
The digital information retention stability of PF14-b-Pison-based memory devices was also explored (Supplementary Figure S9). The memory cells could maintain either an ON or OFF state for at least 10 000 s under a bias of −1 V and exhibited high ON/OFF ratios of 105–106, demonstrating that the studied memories have stable resistive switching characteristics to distinguish each memory (that is, different resistance) state. Furthermore, the cumulative probability of the ON and OFF state switching current for the studied memory cells is presented in Supplementary Figure S10. Stable and reliable current responses were also observed. The abovementioned results clearly indicate that the thermally annealed PF14-b-Piso10 thin film exhibited volatile SRAM memory behavior, whereas the other studied block copolymers showed nonvolatile WORM characteristics. The thermal annealing process, more importantly, can efficiently improve the stability and reproducibility of the memory cells. The threshold voltage, the ON state current and the ON/OFF ratio, moreover, can be controlled through the PF/Piso block ratio. High-performance memory devices with tunable charge storage volatility can thus be achieved through molecular design, and the unique morphological characteristics of block copolymers provide a facile platform for enhancing the resistive switching properties.
The energy level diagrams of the studied block copolymer-based memory devices with low (that is, PF14-b-Piso10) and high (that is, PF14-b-Piso100) Piso contents are shown in Figure 6a and b, respectively, to elucidate the conduction mechanism of the resistive switching. On the basis of the studied device configuration of ITO/PF14-b-Pison/Al, the energy barrier between the bottom ITO contact and HOMO level of the PF14 donor (0.68 eV) is much smaller than that between the Al electrode and the LUMO level of the Piso100 acceptor (1.34 eV), indicating that the device is initially driven by hole carrier injection from ITO to the HOMO level of the active materials. The trapped holes in PF can then attract the opposite charge carriers and electrons, under an applied electric field. Electric field-induced charge transfer between electron donors (that is, PF) and acceptors (that is, Piso) may then occur, and electrons can be transferred from the PF rods to the Piso coils by excitation under a sufficiently high applied voltage, especially in an environment characterized by a high Piso content. Such charge transfer interaction leads to a stable charge separation state, and effective conducting channels would be established in the active layer with reduced charge transport resistance.32 The resistive switching characteristics of the studied memories are affected by the donor–acceptor charge transfer, energy barrier and morphology of the studied block copolymers. As the content of Piso coils (PF14-b-Piso20, PF14-b-Piso60, and PF14-b-Piso100) increases, the polymer active layer exhibits a stronger D–A charge transfer interaction to induce more charge carriers and a larger phase separation d-spacing to prevent hole–electron recombination, creating the stable ON state of the memory device. Nonvolatile memory characteristics, thus, were obtained. In contrast, PF14-b-Piso10-based active layer could not stabilize the induced charges after programming such that the device would return to the OFF state after turning off the power. The energy barrier between ITO and PF14-b-Piso10 is not deep enough to keep the charge from returning, and the microphase domain separation is not large. It should be noted that the obtained HOMO levels of PF14, PF14-b-Piso10, PF14-b-Piso20, PF14-b-Piso60, PF14-b-Piso100 and Piso100 were −5.48, −5.55, −5.74, −5.84, −6.06 and −6.24 eV, respectively. Thus, the energy barrier increased with an increase in the Piso block length. Furthermore, the d-spacing values of PF14-b-Piso10, PF14-b-Piso20, PF14-b-Piso60 and PF14-b-Piso100 were 16.8, 20.8, 24.4 and 29.2 nm, respectively. As the Piso block length increased, both the energy barrier and microphase separation domain were enhanced. Thus, the trapped carrier change could not return to the original state and thus remained in the high conducting state, indicating nonvolatile memory characteristics.
The J–V curves obtained from the PF14-b-Pison-based memories, on the other hand, were theoretically fitted to both the OFF and ON states in the negative voltage regions (Figure 6c and d and Supplementary Figure S11). During the early stages of scanning, the current density increased linearly with the progressive increase in the voltage bias, meaning that the charge transport is governed by the Ohmic contact model. The probed J–V characteristics, nevertheless, were significantly altered under a higher applied bias in the OFF state, and a critical switching point (that is, threshold voltage) between the ON and OFF states was reached. In this operating region, the J–V curves in the logarithmic plots are linear, with slopes of ~2.18, 2.28, 2.34 and 2.43 for PF14-b-Piso10, PF14-b-Piso20, PF14-b-Piso60 and PF14-b-Piso100, respectively. It should be noted that a slope greater than 2 indicates that the switching behavior in the OFF state qualitatively matches the trap-associated space-charge-limited-conduction model,33 meaning that the holes are injected into the active layer of the memory cell and captured by hole transport/trapping sites (PF) and then induce several electrons in electron transport/trapping sites (Piso) via a charge transfer interaction. The induced counter space charge near the electrode indeed limits the escape of charge carriers from the trapping sites. In the ON state, the plot of log(J V−1) versus V1/2 showed a linear relationship (inset of Figure 6c and d), suggesting that the trap-assisted Poole–Frenkel emission mechanism dominated the low-resistance state. The occurrence of Poole–Frenkel emission is likely owing to the charge transport of the PF14-b-Pisons-filled charge traps to form the trap-free environment.34
We demonstrated the formation of a donor–acceptor diblock copolymer system whose resistive switching behaviors can be manipulated for efficient digital information storage. Stretchable memory devices, moreover, were fabricated with volatile SRAM and nonvolatile WORM characteristics using PF14-b-Piso10 and PF14-b-Piso60 as the active materials, respectively. The stretchable devices were fabricated through a pre-strain method,22 a common technique for generating organic stretchable electronics, including light-emitting diodes,35 solar cells,36 and memories;22 the device configuration is illustrated in Figure 7a. Figure 7b–g and Supplementary Figure S12 show the J–V curves of PF14-b-Piso10- and PF14-b-Piso60-based stretchable resistive memory devices under tensile strains ranging from 0 to 50%. SRAM and WORM characteristics with well-defined electrical responses could be observed for the PF14-b-Piso10 and PF14-b-Piso60 devices, respectively, which are identical to those of devices prepared on an ITO glass substrate. Notably, stable memory behaviors could be obtained with an ON/OFF memory ratio of up to 105 at −1 V, suggesting that our stretchable memories can be stably operated as the active layer is elongated. It should be noted that the threshold voltage of both the PF14-b-Piso10- and PF14-b-Piso60-based stretchable devices decreased as the tensile strain was increased because the active layer thickness was slightly reduced during stretching.
More importantly, the durability of the programmed memory parameters, such as the ON/OFF current ratio and threshold voltage, under various stretching conditions were investigated (Figure 8 and Supplementary Figure S13). Both the PF14-b-Piso10- and PF14-b-Piso60-based devices were tested under 200 stretch/release cycles at 20 and 40% applied strain to determine the stability and reproducibility of the stretchable resistive memories. The ON/OFF ratio and threshold voltage of the PF14-b-Piso10 and PF14-b-Piso60 stretchable memories decreased slightly during the continuous stretching cycles because the conducting channel in the active layer may have been damaged under strain. Nevertheless, these electrical properties were still comparable to those of the device fabricated on a rigid ITO substrate, indicating the potential of the polymer-based devices for stretchable electronic applications.
The changes in the electrical properties of the stretchable memory devices may be related to the thin film morphology of the active layer. Figure 9 and Supplementary Figure S14 show the AFM topographies of PF14-b-Piso10 and PF14-b-Piso60 thin films under strains ranging from 0 to 40%. Generally, no distinct cracking was observed on the surface under strain, explaining why the active layer could maintain its electrical properties under stretching. The formation of the crack-free surface under stretching may have been owing to the protection against buckling afforded by PDMS during the pre-strain treatment (Supplementary Figure S15).22, 36 Nanostructures self-assembled by the PF rods, however, could not be obtained in the unstretched films (that is, 0%; relax back from pre-strain) of either PF14-b-Piso10 and PF14-b-Piso60 because the thin films were relatively compressed. As the tensile strain was applied (that is, 20 or 40%), nanofibrillar PF channels were clearly observed on the surface, comparable to those formed on the rigid substrate (Figure 3). It should be noted that additional wrinkles perpendicular to the strain direction were observed on the 40%-restrained PF14-b-Piso10 surface because the soft coil segment composition of PF14-b-Piso10 was low, reducing its thin film ductility.
Conjugated rod-coil diblock copolymers, poly[2,7-(9,9-dihexylfluorene)-block-poly(pendent isoindigo) (PF14-b-Pison, n=10, 20, 60 and 100) consisting of main-chain conjugated PF donors and pendent electron-withdrawing isoindigo were successfully prepared. Tunable surface structures and polymer properties were achieved by controlling the PF/Piso coil-to-rod ratio. Self-assembled fibrillar nanostructures as well as effective charge transport channels in the polymer thin films were formed through the thermal annealing process, leading to stable resistance switching behavior for memory device applications. The studied resistive memories exhibited volatile SRAM (PF14-b-Piso10) and nonvolatile WORM (PF14-b-Piso20, 60, 100) characteristics with an ON/OFF ratio of up to 106 and a data retention time over 104 s on the basis of PF14-b-Pisons with different lengths of the Piso segment. The results indicate that stable digital information storage electronics could be achieved and the charge storage volatility was easily manipulated by tuning the PF/Piso ratio. More importantly, the memory cells were integrated on a PDMS substrate to make the devices stretchable. Reliable and reproducible electrical characteristics of both SRAM- and WORM-type memory were exhibited under an applied tensile strain ranging from 0 to 50%, demonstrating the potential for high-performance wearable electronic applications.
We acknowledge financial support from the Ministry of Science and Technology of Taiwan.
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