Miao
Tang
a,
Ke
Lei
a,
Xingying
Zhao
a,
Xifeiling
Hu
a,
Quansheng
He
a,
Ke
Zhang
a,
Xianhui
Ma
a,
Hualiang
Ni
c,
Yousheng
Shu
a and
Zili
Li
*b
aJinshan Hospital, Institute for Translational Brain Science, Fudan University, Shanghai 200433, China
bSchool of Information Science and Technology, Fudan University, Shanghai, 200433, China. E-mail: lizili@fudan.edu.cn
cAoyi Information Technology Co., Ltd, Shanghai 200433, China
First published on 3rd March 2025
Flexible substrate materials with high adhesion, high stretchability, and low impedance are essential to ensure long-term stable acquisition of electrophysiological signals with less tissue inflammation. Polydimethylsiloxane is a promising candidate owing to its inherent flexibility and biocompatibility; however, its poor adhesion to the skin and excessive stiffness of tissue interfaces limit its application in this field. To address these challenges, we developed a flexible electrode system based on crosslinked block polyborosiloxane and carbon nanotube (C-PBS/CNT) elastomers carrying hydroxyl groups through a thiol–ene reaction. The composite exhibits enhanced adhesion to both the skin and skull, high stretchability, and tunable stiffness ranging from 10 to over 200 kPa, enabling adaptability to the long-term monitoring of epileptic activity and other application scenarios. Moreover, the C-PBS/CNT composite elastomer demonstrated excellent self-healing performance owing to its dynamic boronate ester and hydrogen bonds. The packaged C-PBS/CNT electrode demonstrates low impedance for efficient multi-channel acquisition of epileptic activity under humid conditions. These innovations enable a precise analysis of cortical epileptic-activity propagation and provide an essential technological platform for the prediction and treatment of epileptic seizures, paving the way for next-generation wearable biomedical devices.
A polydimethylsiloxane (PDMS)-based electrode can mitigate this mechanical mismatch owing to its excellent flexibility and biocompatibility.6–9 However, its intrinsic hydrophobicity and weak adhesion lead to delamination during seizure-induced movements, thereby compromising signal fidelity. High-energy treatment is an important strategy to introduce hydrophilic moieties on the PDMS substrate and enhance adhesive properties.10–12 Nevertheless, the hydrophilic surface recovers its hydrophobicity upon contact with air.10 An alternative strategy to create permanently hydrophilic PDMS and increase its adhesive properties is surface grafting with hydrophilic polymers13–15 through surface oxidation treatment and subsequent chemical reactions. However, this modification process is time-consuming and tedious, and the structure of the resulting PDMS-based materials is uncontrollable. In addition, the chemical grafting process is usually implemented under organic solution conditions, limiting its application in biological samples. Therefore, it is urgent to prepare PDMS-based electrodes with controllability and high adhesive performance in the film state using convenient methods.
In addition, the PDMS elastomer is an intrinsic electrical insulating material, and incorporating conductive carbon nanotubes (CNTs) into polymer matrices is a promising strategy for enhancing the electrical conductivity and mechanical adaptability owing to their extraordinary strength, electrical conductivity, and low percolation thresholds to form conductive paths16–18 and further expand their potential for biosignal monitoring.16,19 Nevertheless, conventional PDMS/CNT composites suffer from weak interfacial strength between CNT and PDMS substrate, arising from the great tendency of aggregation of CNT20–22 and poor adhesion of commercial silicone (Sylgard 184).19,23 Generally, an interface of a polymer layer is introduced to modify the CNT, increasing the adhesion with PDMS (hydrophilic treatment) and eliminating CNT detachment from the electrode substrate. However, these electrodes are not adhesive enough to tolerate the large mechanical deformations that occur in many neural activities and lack self-healing performance. Moreover, the modification process is tedious, and the interlocking polymer is mostly limited to conductive poly(3,4-ethylenedioxythiophene):poly(styrene sulfonate) (PEDOT:PSS).8 Introducing the hydroxyl groups into the backbone of PDMS in the molecular structure can integrate both flexibility and adhesion for electrode applications. The hydroxyl groups enhance the dispersion of CNT in PDMS through the hydrogen bonds and improve adhesion to the tissue surface, offering a long-lasting functional neural interface. We prepared a block PDMS elastomer with dangling hydroxyl groups on the backbone to obtain an adhesive electrode.24,25 However, the block PDMS suffers from low mechanical properties, leading to poor film-forming capability and weak mechanical strength for peeling.
Herein, we address these compromises by fabricating a self-healing and high-adhesive conductive electrode with crosslinked block PDMS-based elastomers doping CNT nanomaterials for chronic epilepsy monitoring. The resulting crosslinked block polyborosiloxane (C-PBS) elastomers with dangling hydroxyl groups on the backbone were synthesized through a thiol–ene click reaction. The mechanical and adhesive properties can be manipulated by the feed ratio of the component and crosslinker. This system integrates tunable mechanical properties with stiffness adjustable from 10 to over 200 kPa and meets diverse application demands. The electrode exhibits strong adhesion to both skin and neural tissues, supporting stable operation even under humid sweating conditions. Additionally, the self-healing capabilities arising from the dynamic equilibrium of the crosslinking networks enhance the durability and operational lifespan. CNTs acted as the conducting channel in the composite and endowed a low impedance, sensitive, and stable interface for the electrode. This innovative C-PBS/CNT composite offers high stretchability, high adhesion, and multi-channel recording capabilities, representing a significant advancement in polymer-based biosignal interfaces and paving the way for robust, long-term solutions for epilepsy research and clinical applications.
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Fig. 1 Schematic of the synthesis and self-healing mechanism of C-PBS. (a) Synthetic route and chemical structure of C-PBS. (b) Types of crosslinking points in C-PBS and the self-healing mechanism. |
The chemical structure of the elastomer was first characterized by Fourier Transform Infrared (FTIR) measurement. Fig. 2a presents the FTIR spectra of v-PDMS, DTT, D4, the premixture, and the final C-PBS. The disappearance of the CC stretching vibration (1610 cm−1) from v-PDMS and D4, along with the disappearance of the –SH stretching vibration (2549 cm−1) from DTT after the thiol–ene reaction,24 confirms the near-complete consumption of functional groups during polymerization and formation of the block PBS with dangling hydroxyl groups and crosslinking network with cyclotetrasiloxane as a crosslinking point. Additionally, the broad peak at 3450 cm−1 is assigned to the hydroxyl group, and its intensity became weak after forming the dynamic network with BA. These results demonstrate the formation of dynamic boronate ester bonds in the elastomer, further supporting the structural formation of C-PBS. The progression of the reaction can also be monitored by observing the modulus variation. Before the reaction, the premixture exists in a liquid state without shape, while the final C-PBS demonstrates notable shape manufacturability and stretchability. Mechanical testing of the C-PBS samples reveals that the tensile strength can be tailored by adjusting the feed ratio of v-PDMS to DTT. Remarkably, the material exhibits an elongation at break exceeding 1000%, as shown in Fig. 2b. Moreover, the incorporation of D4 enhances the tensile strength of C-PBS, and this effect is particularly pronounced in samples prepared with a reaction ratio of 1
:
1.2 for v-PDMS to DTT. This phenomenon is likely owing to the increased interaction between PBS chains and D4, where the external thiol groups can react with more double bonds, forming a covalent network with high density. Furthermore, the influence of crosslinker content on the mechanical properties was explored, as shown in Fig. 2c and d. The mechanical strength gradually increases with an increase in D4 content, accompanied by a decrease in elongation. This can be attributed to the high crosslinking density with more D4 crosslinkers. These results corroborate the schematic illustration in Fig. 1, confirming the successful synthesis of the C-PBS elastomer. Based on these results, a feed ratio of 1
:
1.2 is selected for further investigation of the elastomer composite, as it provides an optimal balance of mechanical properties and dispersibility for further introduction of nanofillers.
The mechanical properties of the C-PBS/CNT composites were regulated by CNT contents and the D4 crosslinker, as shown in Fig. 3a and b. The resulting conductive composite elastomers carrying dynamic networks exhibited a wide range of tensile stress from 30 kPa to 230 kPa by controlling the CNT contents, as shown in Fig. 3a. Meanwhile, the addition of D4 further increased the tensile stress of C-PBS-1.2–3/CNT, indicating that the crosslinking density and mechanical properties could be further tuned by manipulating the formulation, which is consistent with the aforementioned results. The abundant hydrogen bonding in C-PBS also imparts unique self-adhesiveness to various substrates, enabling stable and durable interfaces for electrodes. Peeling apart materials is an important technique for characterizing adhesion properties. The peeling strength of C-PBS-1.2 prepared with different D4 amounts was quantified on the skull (Fig. S1†), as shown in Fig. 3c. The peeling strength between C-PBS-1.2 and the skull reached as high as 250 N m−1, whereas Scotch tape exhibited no adhesion to the skull. It is noteworthy that the adhesion property is lower with the addition of CNT because it blocks the contact of hydroxyl groups with the surface, as shown in Fig. 3d. Considering the service conditions of flexible electrodes with softness and high adhesion, we chose C-PBS-1.2–3 with dynamic boronate ester bonds as the polymer matrix for preparing conductive electrode (C-PBS-1.2–3/CNT-4) with the addition of 4 mg CNT.
Owing to the mobility of PBS chains as well as the abundant hydrogen bonds and boronate ester bonds within the polymer matrix, C-PBS demonstrated exceptional intrinsic self-healing capabilities.24 To quantify this spontaneous healing behavior, stress–strain curves of C-PBS-1.2–3/CNT-4 composite at various healing times were recorded, as shown in Fig. 3e. Mechanical healing efficiency can be calculated as the ratio of the restored stress to its original stress.28 The stress gradually recovers to a high efficiency of 92% at room temperature, highlighting the ability of the composite to recover its mechanical properties after suffering cracks or fractures. Conductivity is another important feature for evaluating the capability of electrodes, and lower contact impedance is necessary to obtain high-quality signals. To further investigate the autonomous self-healing ability of the C-PBS/CNT electrode, the self-healing of electrical properties of conductive C-PBS/CNT was further evaluated by in situ monitoring of its resistance. When the elastomer material was cut with a razor blade, the circuit was interrupted, resulting in resistance instantly increasing to the megaohm range (Fig. 3f). Remarkably, within only 2 seconds, the resistance returned to its original value without any external stimulus. Resistance was also recorded after multiple cutting and healing cycles, demonstrating consistent recovery (Fig. 3f). This rapid and complete restoration of electrical conductivity is attributed to the autonomous reconstruction of the conductive network induced by the hydrogen bonding interactions, dynamic boronate ester bonds, and dynamic movement of the polymer chains.28,29 Compared to previously reported self-healing electrodes, which often fail to fully recover conductivity or require an extended time for healing, the conductive C-PBS/CNT in this study offers a significant improvement. The dynamic nature of the network within the C-PBS matrix not only facilitates the reconstruction of the network for mechanical properties but also ensures efficient reconnection and transport of the conducting network for conductivity after cutting. This unique combination of abundant hydrogen bonding and CNT dispersion enables the rapid and robust recovery of both mechanical and electrical properties, making conductive C-PBS/CNT a promising electrode candidate for self-healing electronic applications.
As the electrode is applied to long-term adhesion and even sweating scenes, the peeling test of C-PBS/CNT was characterized under saline conditions to simulate the actual application scenario of the human body, as shown in Fig. 3g. The electrode exhibits a high peel strength of 60 N m−1 on tissue under dry conditions, and the strength gradually decreases as the CNT content increases, for example, from 60 N m−1 with 4 mg to about 30 N m−1 with 6 mg CNT. This can be attributed to the fact that the presence of CNT blocks the bonding interaction with the adherends.30 Moreover, even after soaking in saline, the C-PBS-1.2–3/CNT-4 composite maintained a peeling strength of 10 N m−1 on tissue, outperforming many reported underwater adhesives and even exceeding the adhesion strength of Scotch tape in air. It is commonly believed that PBS may hydrolyze in aqueous environments,31 leading to adhesion failure. However, in this study, the D4 in the C-PBS matrix provides robust chemical crosslinking, which mitigates hydrolysis and ensures stable adhesion under wet conditions. This self-adhesiveness allows for stable and tight contact of soft electronics with interfaces, such as skin, skull, and even complex curved surfaces, as shown in Fig. S2.† Robust adhesion even after prolonged soaking in saline ensures long-term durability in wet environments, including activities in bathing or implantable applications. To further evaluate its performance under dynamic conditions, we conducted tests involving long-term impedance monitoring (Fig. 3h) and twisting (Fig. 3i). The C-PBS/CNT-4 composite demonstrates a decreasing impedance with adhesion time, which can be as low as 62 kΩ. A similar trend can be observed for the C-PBS/CNT-6 composite, as shown in Fig. S3.† Furthermore, the contact impedance gradually decreases with duration time in the test frequency range under dry conditions. This can be attributed to the dynamic C-PBS and CNT networks, resulting in closer contact and lower contact impedance for a longer time. However, compared with commercial electrodes, it shows an upward trend over time (Fig. S4†). This is related to the conduction principle of commercial electrodes. The loss of water in the hydrogel leads to an increase in impedance. Therefore, C-PBS/CNT composites with low impedance, high adhesion, and self-healing properties are suitable for bioelectronic applications that require stable and durable interfaces. After twisting at different angles, the resistance of the C-PBS/CNT composite quickly returned to its original state, demonstrating its excellent resistance to dynamic stresses. This is a critical property for applications in dynamic environments.
The biocompatibility of C-PBS/CNT was also evaluated to extend the service life and ensure safety, as it is indispensable for on-skin devices; PDMS with biocompatibility as a control sample has been well documented.32 The C-PBS/CNT composites could adhere to the skin of C57 mice for 2 months to explore the irritation without bandages (Fig. S5†). The hematoxylin–eosin staining skin samples underneath the C-PBS/CNT composites showed no more inflammatory cell infiltration compared with normal skin nearby, further confirming the excellent biocompatibility of the C-PBS/CNT composites.
The capability of the C-PBS/CNT probe to capture characteristic neural signals across stages of epilepsy was systematically explored, as shown in Fig. 4c–f. To further evaluate the capability of detecting signals during epileptic seizures, an assessment of the seizures in mice was implemented with a C-PBS/CNT electrode. This demonstrated remarkable stability during chronic epilepsy monitoring with fewer motion artifacts. Particularly, the C-PBS/CNT electrode maintains conformal contact on mouse skulls even during movement, enabling continuous EEG recordings from anesthetized to awake states (Fig. 4c and d) and during epileptic seizures (Fig. 4c–e). Fig. 4f shows the power spectral density (PSD) of mouse brain activity under anesthetized, awake, and epileptic conditions. Low-frequency dominance (0–4 Hz) is observed in the anesthetized state, while the awake state exhibits broader frequency activation with increased mid- and high-frequency power (10–50 Hz). The epileptic state shows elevated high-frequency power (30–80 Hz), reflecting abnormal neuronal synchronization. We repeated these experiments in 3 mice and obtained similar results. These acquired characteristic oscillation signals are favorable for speculating certain states of epilepsy. Nevertheless, conventional EEG systems are limited to anesthetized animals owing to the difficulty of maintaining stable contact during movement. This robust adhesion ensures the long-term reliability of C-PBS/CNT electrodes, conquering the limitations of commercial electrodes, which often fail because of their size, stiffness, and poor adaptability to dynamic environments. Therefore, the C-PBS/CNT electrode provides a versatile and reliable solution for advancing epilepsy research and improving disease management in both animal and clinical settings.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d5nr00171d |
This journal is © The Royal Society of Chemistry 2025 |