Zichao
Wang†
a,
Xuan
Zhang†
*a,
Xuehua
Zhou
a,
Mingze
Liu
a,
Xuefeng
Zhu
a,
Mingchao
Zhang
b,
Xuzi
Yang
a,
Yinglai
Hou
*a,
Yuzhang
Du
a and
Jie
Kong
*a
aMOE Key Lab of Materials Physics and Chemistry in Extraordinary Conditions, Shaanxi Key Lab of Macromolecular Science and Technology, School of Chemistry and Chemical Engineering, Northwestern Polytechnical University, Xi’an, 710072, P. R. China. E-mail: zhangxuan@nwpu.edu.cn; houyinglai95@mail.nwpu.edu.cn; kongjie@nwpu.edu.cn
bDepartment of Materials Science and Engineering, National University of Singapore, 117575, Singapore
First published on 24th September 2025
The creation of adaptive memory based on soft matter, similar to the brain, is an attractive and challenging research area. Hysteresis is closely related to adaptive memory because it involves a system's ability to retain and utilize information about its past states or inputs to influence its current and future behavior. To achieve adaptive memory control, it is highly desirable to develop stimuli-responsive hydrogels with a tunable hysteresis in the volume phase transition. Herein, we propose a one-pot synthesis method to develop environmentally adaptive memory by preparing dual-responsive hydrogels (e.g., poly(N-isopropylacrylamide-co-acrylic acid)-g-methylcellulose). The range of the hysteresis window in temperature-dependent shape morphing can be adjusted from approximately 0 °C to 17.6 °C by changing the pH stimulus. Furthermore, the thermal hysteresis windows adapt to the surrounding temperature autonomously. The P(NIPAm-co-AAc)-g-MC hydrogel can maintain a series of small hysteresis loops, which are suitable for memorizing multiple states. Applications in microvalves, hydrogel patterns and smart windows are successfully demonstrated, leveraging the intrinsic hysteresis behavior of the hydrogels. The memory function can switch between memorizing and forgetting behavior, and the memory window adapts to environmental stimuli autonomously. This work contributes an innovative strategy to the development of adaptive memory based on soft materials, paving the way for more intelligent systems.
New conceptsThe creation of adaptive memory based on soft matter, similar to the brain, is an attractive and challenging research area. Hysteresis can involve a system's ability to retain its past states to influence its current and future behavior. However, most reported hysteresis of stimuli-responsive materials fails to exhibit switching between states with hysteresis and without hysteresis after fabrication, which means the memory function is unable to switch between memorizing and forgetting behavior. Moreover, the memory window of hysteresis is unable to adapt to environmental stimuli (e.g., pH and temperature) autonomously or be adaptively adjusted. Herein, we propose a one-pot synthesis method to develop environmentally adaptive memory by preparing dual-responsive hydrogels (e.g., poly(N-isopropylacrylamide-co-acrylic acid)-g-methylcellulose). The hysteresis window in temperature-dependent shape morphing can be adjusted from approximately 0 °C to 17.6 °C by changing the pH stimulus, which shows that the memory function can switch between memorizing and forgetting behavior. Furthermore, the thermal hysteresis windows adapt to the surrounding temperature autonomously. The P(NIPAm-co-AAc)-g-MC hydrogel can maintain a series of small hysteresis loops, which are suitable for memorizing multiple states. This work contributes an innovative strategy to the development of adaptive memory based on soft materials, paving the way for more intelligent systems. |
In recent years, increasingly advanced soft matter with memory functions has been the focal point in the pursuit of new material applications. Shape memory and stimuli-responsive materials have attracted major efforts in the development of material properties that can be changed on demand by imposed stimuli, such as pH, temperature, light, magnetic field, electrical and mechanical stimuli.5,6 Shape memory polymers (SMPs) exhibit a permanent shape at low temperature (below the transition temperature), deform at a high temperature (above the transition temperature), and maintain the deformed shape after cooling down (below the transition temperature). SMPs turn back from the deformed shape to the permanent shape upon reheating. Recently, researchers utilized a single medical-grade SMP to combine shape morphing and SMP behaviors at physiological temperatures to yield smart implants with precise control over dimensions for tissue repair and regeneration.7 Such a shape memory effect has been found in a variety of polymers, such as liquid crystalline elastomers, amorphous polymers and semicrystalline polymers.5 The switching temperature region of SMPs can determine the service temperature of the materials, which is a crucial parameter for the application of SMPs. From the molecular viewpoint, the switching temperature region is generally related to the melting temperature of semicrystalline SMPs or the glass transition temperature of amorphous SMPs.7–9 The switching temperature region of SMPs can be effectively tuned by varying the photo-crosslinking degrees of the polymer network,10 copolymer compositions9 and material compositions.11–13 However, these strategies for memory function do not enable switching between memorizing and forgetting behavior, and the switching temperature region fails to be adaptively and reversibly adjusted after fabrication.
A wide range of stimuli-responsive materials that respond to many different types of stimulus has been fabricated and has found promising applications in grippers, sensors, valves, soft robotics and biomedical applications.14 Recently, multifunctional conductive hydrogels comprising alginate, MC and acid-functionalized carbon nanotubes fabricated by 4D printing were demonstrated as flexible strain sensors. Furthermore, the synergistic effect of electrical cues and the in situ self-folding ability of these hydrogels enabled sutureless neurorrhaphy and superior neural regeneration.15 Stimuli-responsive materials typically exhibit path-independent, non-volatile behavior, with a one-to-one correlation between the environmental stimulus and their material properties. For example, the material reliably demonstrates a prescribed property at a given temperature, regardless of its prior thermal history. However, these materials fail to achieve memory functionality due to their history-independence. In intelligent systems, memory enables the system to learn from past stimuli and adjust responses accordingly. Hysteresis-like behavior can provide a mechanism for retaining and weighting past inputs, allowing for adaptable responses. Depending on the environmental history of the material, multiple states of the material can exist under the same environmental conditions.16–18 Hysteresis is an interesting phenomenon, which displays an output depending on both past and present inputs. In addition to ferroelectric and ferromagnetic materials, some soft matter materials such as stimuli-responsive soft materials also exhibit hysteresis.19,20 Such hysteretic properties of soft materials could be used in memory devices. Bistable states of the soft material can exist, resulting in storage of information on physical history in a single environment.21,22 Polymers with large thermal hysteresis can memorize historic information and the memory may be removed by excessive cooling, such as a large thermal hysteresis in volume phase transition, which paves the way for the next generation of microvalves, actuators, drug delivery systems and microrobots.19,23–25 In general, the thermal hysteresis of the LCST, i.e. the difference in the volume phase transition temperatures of the heating and cooling processes, is very small due to the rapid dissolution of the polymer chains in their shrunken state.26 It has been reported that polymers with large thermal hysteresis can memorize changes in their state and that the memory may be deleted by excessive cooling.27,28 Recently, studies have reported several methods to enhance the thermal hysteresis of materials, which include the incorporation of MC19,29,30 and amphiphilic groups,31 control of stereo-regularity,32 utilization of host–guest interactions33 and changing of the electrostatic crosslinker.34 These studies mainly concerned sol–gel transitions25,29 or transmittance changes.16,29,30,34 To achieve programmable volume control, it is highly desirable to develop stimuli-responsive hydrogels with a large hysteresis capable of memory in the volume phase transition. Mori et al. have previously reported a hydrogel prepared with an α,α-disubstituted vinyl monomer with amphiphilic substituents, which exhibited a 5 °C thermal hysteresis in its volume change.24 This improved hysteresis was possible because the material was capable of forming a metastable aggregate due to its enhanced intra/intermolecular interaction. Dowan et al. reported the preparation of a stimuli-responsive hydrogel by incorporation of MC, which showed a 10 °C thermal hysteresis in its volume phase transition.22 While they demonstrated the capability of influencing a relatively large thermal hysteresis, the materials failed to be switched between exhibiting and not exhibiting hysteresis once fabricated,19,21,22,34 which means the memory function is unable to switch between memorizing and forgetting behavior. Moreover, most of the previous studies showed that the memory window of hysteresis is unable to adapt to environmental stimuli (e.g. pH and temperature) autonomously or be adaptively adjusted after fabrication. To achieve adaptive memory control, it is highly desirable to develop stimuli-responsive hydrogels with a tunable hysteresis capable of adaptive memory in the volume phase transition. Unlike classic synthetic SMPs and stimulus-responsive materials, which are limited to fixed responses, living organisms exhibit dynamically adaptive responses influenced by the intensity, repetition, and history of stimuli. Therefore, adaptive memory that advances “material intelligence” and progressively life-like properties is an emerging need, and yet a grand challenge.
In this study, we propose a one-pot synthesis to fabricate dual-responsive hydrogels with adaptive memory that exhibits environmental adaptive memorizing behavior. The dual-responsive hydrogels poly(N-isopropylacrylamide-co-acrylic acid)-g-methylcellulose (P(NIPAm-co-AAc)-g-MC) and poly(N-n-propylacrylamide-co-acrylic acid)-g-methylcellulose (P(NNPAm-co-AAc)-g-MC), with tunable thermal hysteresis, were prepared by introducing P(NIPAm-co-AAc) or P(NNPAm-co-AAc) chains onto MC backbones and concurrently crosslinking the P(NIPAm-co-AAc) or P(NNPAm-co-AAc) (Fig. 1(a)). The adaptive memorizing behavior is achieved based on the MC backbone and dual responsiveness. It was anticipated that stabilized aggregates would be formed above the lower critical solution temperature (LCST) due to the intermolecular interactions of the MC backbone. Such stabilized aggregates are very important for achieving a large thermal hysteresis in volume change.17 The memory window of hysteresis can be tuned by varying the LCST of the P(NIPAm-co-AAc)-g-MC or P(NNPAm-co-AAc)-g-MC hydrogels upon environmental pH stimulation. The memory function is able to switch between memorizing and forgetting behavior, and the memory window can be adaptively and reversibly adjusted after hydrogel fabrication (Fig. 1(b)). Moreover, the different partially contracted states of the hydrogels are also maintained, resulting in a series of relatively small thermal hysteresis loops, which are suitable for adaptively memorizing more states. This strategy of developing adaptive memory based on a tunable phase transition hysteresis might be applied to a broad range of stimuli-responsive soft materials.
O stretching band of PNIPAm at 1637 cm−1 can also be observed. The successful synthesis of the P(NIPAm-co-AAc)-g-MC network is shown by above observations.
To evaluate the tunable thermal hysteresis of the fabricated P(NIPAm-co-AAc)-g-MC hydrogel, the swelling ratio was measured as a function of temperature (Fig. 2). Prior to measuring the swelling ratio, the hydrogel was maintained for enough time (e.g., 5 hours) at a specific temperature to fully reach equilibrium.37 When the P(NIPAm-co-AAc)-g-MC hydrogel was exposed to a solution of pH 4, the hydrogel showed a dramatic volume phase transition close to ∼31 °C (its LCST) during heating (Fig. 2(a)). This transition was found to be fully reversible, but almost no hysteresis is observed. At pH 4.5, the swelling ratio of the P(NIPAm-co-AAc)-g-MC remains unchanged until 38 °C (Fig. 2(b)). Upon heating, an abrupt volume shrinkage of the P(NIPAm-co-AAc)-g-MC starts at 39 °C, which is higher than the temperature for the P(NIPAm-co-AAc)-g-MC hydrogel at pH 4. Some of the PAAc repeating units are deprotonated at pH 4.5, leading to the hydrophilic P(NIPAm-co-AAc) backbone. The hydrophilic backbone promotes the hydration of the polymer chains and inhibits polymer aggregation, resulting in an increase in the LCST. During cooling, the thermal behavior of P(NIPAm-co-AAc)-g-MC is different from that observed in the heating process. Surprisingly, at 40 °C, which is below the LCST observed during heating, the swelling ratio of P(NIPAm-co-AAc)-g-MC is still maintained even after 3 days. This means that the reswelling of P(NIPAm-co-AAc)-g-MC is hindered, which is presumably because the intra/intermolecular interactions of the MC backbones lead to thermal hysteresis in the volume change.19 Below 38 °C, the hydrogel begins reswelling, and the initial volume is fully recovered after further cooling to 36 °C. This result clearly demonstrates that the P(NIPAm-co-AAc)-g-MC hydrogel has a thermal hysteresis window, which might pave the way for a memory function. As the solution pH is increased to 5, the LCST continues to increase due to the deprotonation of more PAAc repeating units. The thermal hysteresis window at pH 5 also becomes larger (Fig. 2(c)) compared to that at pH 4.5. This is because the hydrophobic association of MC chains intensifies with increasing temperature, resulting in the formation of junctions.38 In contrast, almost no hysteresis is observed for the P(NIPAm-co-AAc) hydrogel upon varying the pH stimulus (Fig. S2). As the pH solution increased to pH 5.5, pH 6 and pH 7, the LCST continued to increase because more and more PAAc repeating units were deprotonated, and the thermal hysteresis window gradually became wider (Fig. 2(d)–(f)). These results demonstrate that the memory function of the P(NIPAm-co-AAc)-g-MC hydrogel is able to switch between memorizing (with hysteresis) and forgetting (no hysteresis) behavior, and the thermal hysteresis window can be adaptively and reversibly adjusted by pH after hydrogel fabrication. The volume change of the P(NIPAm-co-AAc)-g-MC hydrogel can also be affected by pH stimulation (see SI, relationship between pKa value of the hydrogel and volume change with pH).
In order to explore the generalization of the proposed strategy and expand the application of adaptive memory materials, we chose the monomer N-n-propyl acrylamide (NNPAm) with a lower LCST (∼21 °C)39 to prepare the poly(N-n-propylacrylamide-co-acrylic acid)-g-methylcellulose (P(NNPAm-co-AAc)-g-MC) hydrogel (see SI, materials and preparation). As seen in Fig. 2(g), the P(NNPAm-co-AAc)-g-MC hydrogel shows almost no hysteresis at pH 4. Similar to the P(NIPAm-co-AAc)-g-MC hydrogel, at pH 5, some of the PAAc repeating units are deprotonated, leading to a hydrophilic P(NNPAm-co-AAc) backbone and an increase in the LCST. During heating, an abrupt volume shrinkage of the P(NNPAm-co-AAc)-g-MC starts at 36 °C, which is higher than the temperature for the P(NNPAm-co-AAc)-g-MC hydrogel at pH 4 (LCST ∼21 °C). During cooling, even at 33 °C, which is below the LCST observed during heating, the swelling ratio of P(NNPAm-co-AAc)-g-MC is maintained (Fig. 2(h)). This means that the reswelling of P(NNPAm-co-AAc)-g-MC is hindered due to thermal hysteretic volume change. Below 33 °C, the hydrogel begins reswelling, and the initial swelling ratio is fully recovered after further cooling to 30 °C. The P(NNPAm-co-AAc)-g-MC hydrogel with a thermal hysteresis window is clearly proved by the above experimental results. As the pH solution was increased to pH 5.5, the LCST continued to increase because more PAAc repeating units were deprotonated (Fig. 2(i)). The thermal hysteresis window at pH 5.5 also became larger compared to that at pH 5. Notably, between pH 5 and pH 5.5, the thermal hysteresis window of the P(NNPAm-co-AAc)-g-MC hydrogel is around 37 °C, which is near body temperature, indicating great potential in biomedical fields.
Furthermore, the thermal hysteresis windows of the above hydrogels may autonomously and adaptively change in response to the surrounding temperature without the pH stimulus being adjusted. When the pH of the solutions was fixed at pH 5, the P(NIPAm-co-AAc)-g-MC hydrogel was exposed to solutions with different ionic strengths. The thermal hysteresis window shifted to the lower temperature region with increasing ionic strength (Fig. 3(a)–(c)), which may be due to the salt-out effect.40 Moreover, when the P(NIPAm-co-AAc)-g-MC hydrogel was exposed to a solution of pH 5, and the surrounding temperature was increased to 41 °C followed by a cooling process, the hydrogel exhibited almost no thermal hysteresis (Fig. 3(d)). When the surrounding temperature was increased to 43 °C followed by a cooling process, the hydrogel showed clear thermal hysteresis (Fig. 3(e)). When the surrounding temperature was increased to 47 °C, the hydrogel contracted to become smaller, and the thermal hysteresis window became larger (Fig. 3(f)) compared to that at 43 °C. This is because the hydrophobic association of MC chains intensifies with increasing temperature, resulting in the formation of junctions.38 Similarly, when the P(NIPAm-co-AAc)-g-MC hydrogel was exposed to a solution of pH 6, and the surrounding temperature was increased to 56 °C followed by a cooling process, the hydrogel exhibited almost no thermal hysteresis (Fig. 3(g)). When the surrounding temperature was increased to 58 °C followed by a cooling process, the hydrogel showed clear thermal hysteresis (Fig. 3(h)). When the surrounding temperature was increased to 64 °C, the hydrogel contracted to become smaller, and the thermal hysteresis window became larger (Fig. 3(i)) compared to that at 58 °C. The P(NIPAm-co-AAc)-g-MC hydrogel can maintain a series of relatively small thermal hysteresis loops, which are suitable for adaptively memorizing multiple states. These results demonstrate that the memory function of the P(NIPAm-co-AAc)-g-MC hydrogel is able to switch between forgetting (no hysteresis) and memorizing (with hysteresis) behavior, and the thermal hysteresis window can adapt to the surrounding temperature autonomously.
To further explore the hydrophobic molecular interactions of the P(NIPAm-co-AAc)-g-MC hydrogel in the heating and cooling process, all-atom molecular dynamics (MD) simulations were conducted (Fig. 4(j)). The molecular interaction energies between –CH3 of the MC and MC chains, –CH3 of the MC and PNIPAm chains, and –CH3 of the PNIPAm and PNIPAm chains in the P(NIPAm-co-AAc)-g-MC hydrogel systems were calculated (Fig. 4(k)–(p)). All molecular interaction energies were negative, indicating that the interactions between the molecules were attractive.43 The absolute value of the molecular interaction energies at pH 4 is clearly smaller than that at pH 5, indicating stronger hydrophobic molecular interactions at pH 5. At pH 4, the absolute value of the molecular interaction energy between –CH3 of PNIPAm and PNIPAm chains increases with increasing temperature, and decreases with decreasing temperature (Fig. 4(k)). While at pH 5, the absolute value of the molecular interaction energy between –CH3 of PNIPAm and PNIPAm chains increases with increasing temperature, and remains unchanged with decreasing temperature (Fig. 4(n)). The molecular interaction energy between –CH3 of MC and PNIPAm chains follows a similar trend (Fig. 4(l) and (o)). These results show that the molecular interactions between MC and PNIPAm chains, and PNIPAm and PNIPAm chains might also be contributors to the formation of the thermal hysteresis of the P(NIPAm-co-AAc)-g-MC hydrogel. At pH 4, the absolute value of the molecular interaction energy between –CH3 of MC and MC chains remains unchanged (Fig. 4(m)), probably due to the relatively low temperature range (i.e., 29–35 °C). At pH 5, the absolute value of the molecular interaction energy between –CH3 of MC and MC chains also increases with increasing temperature, and remains almost unchanged with decreasing temperature (Fig. 4(p)), which supports the concept of intra/intermolecular interactions of the MC backbones leading to thermal hysteresis in the volume change.
Regarding the potential applications of the developed P(NIPAm-co-AAc)-g-MC hydrogel, we also envisioned hydrogel patterns capable of adaptive information storage (Fig. 5(c), see SI, hydrogel patterns). This research can be regarded as proof of the concept of hydrogel patterning based on adaptive memory. The pH of the operating conditions may be modified (see SI, the modification of pH of operating conditions). Fig. 5(c) shows that at pH 4 the information “NPU” was visualized upon heating at 32 °C and disappeared upon cooling at 30 °C. When the hydrogel pattern was exposed to a solution of pH 5, the memorized information “NPU” was visualized upon heating at 48 °C and still remained upon cooling at 40 °C. At pH 6, the hydrogel pattern is able to adaptively adjust its memory function and shift the thermal memory window to a higher temperature region. The hydrogel pattern shows the information “NPU” upon heating at 64 °C and this is maintained upon cooling at 53 °C. The results demonstrated that the microvalve and hydrogel patterns based on P(NIPAm-co-AAc)-g-MC are able to switch between memorizing and forgetting behavior, and the memory window adapts to environmental stimuli (i.e., pH) autonomously and reversibly.
The opaque state (0% transmittance) is reached at 52 °C during heating and maintained until 46 °C during cooling. The transmittance was recovered from 43 °C, and the completely transparent state was observed at 37 °C (Fig. 6(c)). The uniformity of light transmittance for the smart window was tested (see SI, uniformity of light transmittance for smart window). The optical transmittance of the window in its partially opaque (e.g. 42% transmittance) state is reached at 49 °C during heating and maintained without applying any energy, rather than the transparent state being recovered (Fig. 6(d)), indicating suitability for the construction of customizable and adaptive smart windows. This smart window may autonomously and adaptively change its optical transmittance according to the outside temperature without the pH stimulus being adjusted. When the outdoor temperature is very high (e.g., 52 °C), the smart window maintains a very low optical transmittance (e.g., 0% transmittance) and relatively large hysteresis window (e.g., in the range of 11.7 °C) during cooling for effectively reducing the indoor temperature. When the outdoor temperature is high, the smart window maintains a relatively low optical transmittance and relatively small hysteresis window during cooling for reducing the indoor temperature and retaining a comfortable level of sunshine at the same time. The hydrogel smart window with tunable memory provides a foundation for novel smart windows for all-weather temperature regulation in diverse climates and will greatly contribute globally to energy conservation of buildings.
Footnote |
| † These authors contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2026 |