Poly(β-hydroxyl amine)s: Valuable Building Blocks for Supramolecular Elastomers with Tunable Mechanical Performance and Superior Healing Capacity

Supramolecular elastomers integrated with high mechanical toughness and excellent self-healing ability offer attractive applications in various fields such as biomedical materials and wearable electronics. However, the multistep preparation process for creating functional polymer precursors and the expensive stock materials required are two factors that limit the widespread use of supramolecular elastomers. Herein, for the first time, poly(β-hydroxyl amine)s generated by amine-epoxy polymerization were used in the development of supramolecular polymer materials. Based on the novel silicon-containing poly(β-hydroxyl amine)s synthesized by the polymerization between 1,3-bis(3-glycidyloxypropyl)tetramethyldisiloxane and 3-amino-1,2-propanediol, dually cross-linked supramolecular elastomers with both hydrogen bonding and metal coordination were achieved, displaying adjustable mechanical properties with the tensile strength varying from 0.70 MPa to 2.52 MPa, respectively. Thanks to the dynamic nature of the supramolecular interactions, these elastomers exhibited favorable hot-pressing reprocessability and excellent self-healing performance, with the healing efficiency reaching up to 98% at 60 °C for 48 h. Potential applications for photoluminescent materials and flexible electronic devices were demonstrated. We believe that its simplicity of synthesis, adjustable mechanical properties, and robust self-healing capacities bode well for future applications of this new supramolecular elastomer.


Introduction
Supramolecular elastomers [1] are elastic networks cross-linked by non-covalent bonds such as hydrogen bonds [2,3], metal-ligand interactions [4,5], host-guest interactions [6,7], and π-π stacking [8][9][10]. Due to the reversible nature of non-covalent interactions, supramolecular elastomers generally have excellent thermoplasticity, enhanced processability, and self-healing properties. Supramolecular elastomers are usually prepared based on one specific supramolecular interaction. Though the mono-cross-linking design is quite straightforward, the tunability of the material properties is limited by the variety of supramolecular interactions. Depending on the strength of the intermolecular interactions, the mechanical strength of the obtained materials ranges from a few tenths of MPa to tens of MPa, while the healing occurs with or without external triggers. In order to improve the design flexibility, mechanical toughness, and self-healing properties of polymeric materials, a cooperative double cross-linking strategy has recently been explored by combining

Characterization and Measurements
The proton nuclear magnetic resonance ( 1 H NMR) spectrum was analyzed on a Bruker Avance 400 MHz spectrometer at 25 • C with CDCl 3 as the solvent and without tetramethylsilane (TMS) as the internal reference for chemical shifts (δ, ppm). The Fourier transform infrared spectrum (FT-IR) was recorded on a Bruker TENSOR 27 infrared spectrophotometer using the KBr pellet technique from the 4000 cm −1 to 500 cm −1 . The resolution was 4 cm −1 and 16 scans with a heating rate of 3 • C/min. Gel permeation chromatography (GPC) indices were detected with a Waters 1515 liquid chromatograph equipped with a 2414 refractive index detector. The column temperature was set at 40 • C and the flow rate of THF was stable at 1.0 mL/min. Differential scanning calorimetry (DSC) was measured using the TA Instruments SDTQ 600 under dry nitrogen flow, and the temperature range was from −140 • C to 100 • C, with a heating and cooling speed of 10 • C/min. For each specimen, two cooling-heating cycles were applied to eliminate thermal history, and the T g was obtained from the second cooling-heating process. The fluorescence (excitation and emission) spectra were performed on a Hitachi F-4500 fluorescence spectrophotometer using a monochromatic Xe lamp as an excitation source. Ultraviolet absorption spectra in a CH 3 OH solution were detected using a TU-1901 Dual Beam UV-Vis spectrophotometer in the wavelength range of 200-700 nm. The transmittance spectra of the elastomer were also recorded by a TU-1901 Dual Beam UV-Vis spectrophotometer in the wavelength range of 200-700 nm. Narrow X-ray photoelectron spectroscopy (XPS) was performed using a Thermo Fisher Scientific (Waltham, MA, USA) ESCALAB 250 spectrometer with a monochromatic Al Kalph (150 W) source. The survey and high-resolution scans were generated at 200 eV pass energy and 30 eV pass energy, respectively. Scanning electronic microscopy images (SEM) and EDS (including elemental mapping) were obtained via a Quanta 250 FEG-SEM device (FEI, Lausanne, Switzerland), and the contents of some elements were recorded simultaneously. The specimens were cut and coated with a thin layer of platinum black before the investigation. Mechanical tensile tests (including the healing and reprocessing tests) of the elastic films were implemented using the Instron 3343 material testing system with a speed of 100 mm/min. For all the tensile tests, the films were cut into several dumbbell-shaped samples with a size of 40 × 4 × 0.8 mm 3 , and at least three parallel tests were conducted. The resistance of the conductive material during the stretching process (speed rate = 5 mm/min) was measured step by step using a CHINT ZTY0105A digital multimeter.

Synthesis of Polymer P1 via the Amine-Epoxy Polymerization
The mixture of 1,3-bis(3-glycidyloxypropyl)tetramethyldisiloxane (7 mmol, 2.544 mL) and 3-amino-1,2-propanediol (7 mmol, 0.638 g) was added to methanol (3 mL), and stirred with a mechanical stirrer at 60 • C for 24 h. Subsequently, the crude mixture was diluted with a small amount of THF and was slowly precipitated into a large amount of petroleum ether, repeated three times. After vacuum drying, the target P1 was obtained. (M w = 10,130, PDI = 2.10.)

Preparation of the Hydrogen-Bonded Elastomer
The solution of polymer P1 in methanol was poured into a Teflon plate mold, dried naturally at room temperature, then dried in a vacuum at 80 • C for 24 h. Finally, the transparent hydrogen-bonded elastomer was obtained.

Preparation of Dually Supramolecular Elastomers (P1-Cu-x/1)
Various amounts of CuCl 2 were introduced into the P1 network to yield dually supramolecular elastomers named as P1-Cu-x/1, where the molar ratio of nitrogen atoms vs. CuCl 2 in P1 was x/1. The preparation of elastomer P1-Cu-3/1 is described as an example. To the solution of polymer P1 (2.26 g, 5 mmol of nitrogen atoms, 1 eq.) in 2 mL of methanol, the solution of CuCl 2 (22.4 mg, 0.167 mmol, 0.33 eq.) in 1 mL of methanol was added. After stirring for 5 min, the mixture was poured into a Teflon mold, dried naturally at room temperature, then dried in a vacuum at 80 • C for 24 h to remove the solvent. Finally, a blue stretchable film was obtained. Following a similar process, all the other dually supramolecular samples were prepared by adjusting the molar ratio of CuCl 2 vs. nitrogen atoms.

Hot-Pressing of the Supramolecular Elastomers
The fractured materials of the elastic films were collected together and introduced into a steel mold (150 × 100 × 0.5 mm 3 ), which was pressed at 50 • C for 20 min under 4 MPa. The tensile measurement was then performed to evaluated mechanical property of the material.

Self-Healing Tests of the Supramolecular Elastomers
The elastomer P1 or P1-Cu-6/1 was cut into dumbbell-shaped specimens with a size of 40 × 4 × 0.8 mm 3 . Each specimen was cut into halves using a blade. The two cut-off pieces were then instantly rejoined at the fracture surfaces and kept at either room temperature or 60 • C for different durations. Tensile measurements on the healed samples were conducted to quantitatively evaluate the self-healing efficiency, which is defined as the ratio of the tensile strength of the healed and original samples.

Preparation of the Photoluminescent Supramolecular Elastomer P1-Eu-x
Various amounts of Eu(NO 3 ) 3 ·6H 2 O were introduced into the P1 network to yield photoluminescent supramolecular elastomers named as P1-Eu-x, where the molar ratio of Eu(NO 3 ) 3 ·6H 2 O vs. nitrogen atoms in P1 was x. Using the preparation of elastomer P1-Eu-20% as an example, to the solution of polymer P1 (1 g, 2.21 mmol of nitrogen atoms, 1 eq.) in 12 mL of methanol, the solution of Eu(NO 3 ) 3 ·6H 2 O (0.22 g, 0.442 mmol, 0.2 eq.) in 2 mL of methanol was added. After stirring at 40 • C for 4 h, the mixture was poured into a Teflon mold, dried naturally at room temperature, then dried in a vacuum at 80 • C for 24 h to remove the solvent. Finally, a stretchable film was obtained. Following a similar process, all the other photoluminescent supramolecular elastomers were prepared by adjusting the molar ratio of Eu(NO 3 ) 3 ·6H 2 O vs. nitrogen atoms.

Preparation of the Conductive Supramolecular Elastomer P1-MWCNT
To the mixture of 3.0 g of hydrogen-bonded polymer P1 in a certain amount of methanol, 10 wt% of multi-walled carbon nanotubes (MWCNT) was added uniformly and dispersed by ultrasound (50 • C, 1.5 h). Afterwards, the mixture was poured into a Teflon mold, dried naturally at room temperature, then dried in a vacuum at 80 • C for 24 h to remove the solvent. Finally, the conductive supramolecular elastomer P1-MWCNT was obtained.

Results
Based on our previous work, poly(β-hydroxyl amine) was selected as the parent polymer to construct dual-cross-linked supramolecular elastomers. As shown in Scheme 1A, this functional polymer is readily prepared via the click polymerization of amine and epoxy monomers at ambient conditions. Along with its polymeric backbone, hydroxyl groups can form hydrogen bonds with each other, while nitrogen atoms with lone-pair electrons can effectively coordinate with metal ions. Both types of non-covalent interactions identify poly(β-hydroxyl amine) as a perfect candidate for constructing supramolecular materials (Scheme 1B). The mechanical behaviors of the obtained networks can be rationally tuned by regulating the metal ion content. Meanwhile, the dynamic natures of the hydrogen bond and the coordination bond give the elastomer outstanding self-healing capabilities.
Based on our previous work, poly(β-hydroxyl amine) was selected as the parent pol-ymer to construct dual-cross-linked supramolecular elastomers. As shown in Scheme 1A, this functional polymer is readily prepared via the click polymerization of amine and epoxy monomers at ambient conditions. Along with its polymeric backbone, hydroxyl groups can form hydrogen bonds with each other, while nitrogen atoms with lone-pair electrons can effectively coordinate with metal ions. Both types of non-covalent interactions identify poly(β-hydroxyl amine) as a perfect candidate for constructing supramolecular materials (Scheme 1B). The mechanical behaviors of the obtained networks can be rationally tuned by regulating the metal ion content. Meanwhile, the dynamic natures of the hydrogen bond and the coordination bond give the elastomer outstanding self-healing capabilities.

Synthesis and Characterization of Polymer P1
The parent polymer was synthesized by the amine-epoxy polymerization between commercially available 1,3-bis(3-glycidyloxypropyl)tetramethyldisiloxane and 3-amino-1,2-propanediol. The former monomer with flexible siloxane units was selected to endow the obtained polymer with a low glass transition temperature, while the latter monomer with hydroxyl groups was selected to increase the density of the hydrogen bonds. The obtained polymer P1 was thoroughly investigated using 1 H NMR, FT-IR and GPC. Figure  1A shows the 1 H NMR spectra of monomer A and polymer P1. In the spectrum of 1,3bis(3-glycidyloxypropyl)tetramethyldisiloxane, the characteristic peaks of the epoxy protons appeared at 2.59, 2.78, and 3.13 ppm, which disappeared after polymerization with 3-amino-1,2-propanediol. In the spectrum of P1, the proton resonances from the methylene groups (g, h) adjacent to the nitrogen atoms overlapped at 2.44-2.82 ppm, while those from the methyl groups (a) adjacent to the silicon atoms appeared at 0.01-0.07 ppm, indicating that the two target motifs were successfully introduced into the polymer chains. The integration ratio of the typical proton signals (a:(g,h):(d,e,f,i):j:i′:e′ = 12:6:9:1:1:2) was in accordance with the theoretical calculation, further confirming the expected polymer structure. Moreover, the FT-IR measurements in Figure 1B showed that the two stretching absorption peaks of the primary amine groups (approximately 3500 and 3400 cm −1 ) in 3amino-1,2-propanediol and the peak of the epoxy groups (915 cm −1 ) in 1,3-bis(3-glycidyloxypropyl)tetramethyldisiloxane disappeared after the polymerization. In addition, The synthesis of silicon-containing poly(β-hydroxyl amine) P1 via the amineepoxy polymerization between 1,3-bis(3-glycidyloxypropyl)tetramethyldisiloxane and 3-amino-1,2propanediol. (B) The preparation of supramolecular poly(β-hydroxyl amine) elastomers cross-linked with both hydrogen bonds (red polygons) and coordination bonds (green arrows and blue circles).

Synthesis and Characterization of Polymer P1
The parent polymer was synthesized by the amine-epoxy polymerization between commercially available 1,3-bis(3-glycidyloxypropyl)tetramethyldisiloxane and 3-amino-1,2-propanediol. The former monomer with flexible siloxane units was selected to endow the obtained polymer with a low glass transition temperature, while the latter monomer with hydroxyl groups was selected to increase the density of the hydrogen bonds. The obtained polymer P1 was thoroughly investigated using 1 H NMR, FT-IR and GPC. Figure 1A shows the 1 H NMR spectra of monomer A and polymer P1. In the spectrum of 1,3-bis(3glycidyloxypropyl)tetramethyldisiloxane, the characteristic peaks of the epoxy protons appeared at 2.59, 2.78, and 3.13 ppm, which disappeared after polymerization with 3amino-1,2-propanediol. In the spectrum of P1, the proton resonances from the methylene groups (g, h) adjacent to the nitrogen atoms overlapped at 2.44-2.82 ppm, while those from the methyl groups (a) adjacent to the silicon atoms appeared at 0.01-0.07 ppm, indicating that the two target motifs were successfully introduced into the polymer chains. The integration ratio of the typical proton signals (a:(g,h):(d,e,f,i):j:i :e = 12:6:9:1:1:2) was in accordance with the theoretical calculation, further confirming the expected polymer structure. Moreover, the FT-IR measurements in Figure 1B showed that the two stretching absorption peaks of the primary amine groups (approximately 3500 and 3400 cm −1 ) in 3-amino-1,2-propanediol and the peak of the epoxy groups (915 cm −1 ) in 1,3-bis(3glycidyloxypropyl)tetramethyldisiloxane disappeared after the polymerization. In addition, the GPC analysis of P1 showed a unimodal distribution with an M w of 10,130 g/mol and a polydispersity index of 2.1. These results confirm the successful synthesis of P1 via amine-epoxy polymerization.
Due to the presence of nitrogen atoms on the backbone, polymer P1 is expected to possess excellent coordination capabilities with electron-deficient metal ions. Therefore, UVvis spectroscopy was used to investigate its coordinating behavior with CuCl 2 (Figure 2A). The UV-vis spectrum of polymer P1 exhibited a major absorption peak at around 231 nm and a minor one at around 291 nm. With the addition of CuCl 2 , the former peak gradually decreased, while the latter almost disappeared. More importantly, a new absorption peak appeared at around 270 nm, and its intensity constantly increased with the addition of CuCl 2 . The difference in UV-vis spectra indicates the change in the electronic environment of the nitrogen atoms and the new UV absorption band could be ascribed to the bonding σ(N) → antibonding d x2-y2 (Cu) charge transfer (according to the literature), demonstrating the effective coordination between polymer P1 and the Cu 2+ ions [25,26].  Due to the presence of nitrogen atoms on the backbone, polymer P1 is expected to possess excellent coordination capabilities with electron-deficient metal ions. Therefore, UV-vis spectroscopy was used to investigate its coordinating behavior with CuCl2 ( Figure  2A). The UV-vis spectrum of polymer P1 exhibited a major absorption peak at around 231 nm and a minor one at around 291 nm. With the addition of CuCl2, the former peak gradually decreased, while the latter almost disappeared. More importantly, a new absorption peak appeared at around 270 nm, and its intensity constantly increased with the addition of CuCl2. The difference in UV-vis spectra indicates the change in the electronic environment of the nitrogen atoms and the new UV absorption band could be ascribed to the bonding σ(N) → antibonding dx2-y2(Cu) charge transfer (according to the literature), demonstrating the effective coordination between polymer P1 and the Cu 2+ ions [25,26]. Unexpectedly, polymer P1 emits blue fluorescence under UV light at 365 nm, even though it does not possess a conventional chromophore. Therefore, the excitation and emission spectra of P1 were studied to verify its fluorescent behavior. As illustrated in Figure 2B, the excitation wavelength appeared at 374 nm, and the emission wavelength appeared at 447 nm. This unconventional fluorescent phenomenon can be explained by the presence of N→Si coordination bonds in the polymeric backbones [27,28]. Photoluminescence would be generated by the through-space charge transfer from the lone electron pair in the nitrogen atoms to the 3d empty orbital of the silicon atoms. Moreover, the  Due to the presence of nitrogen atoms on the backbone, polymer P1 is expected to possess excellent coordination capabilities with electron-deficient metal ions. Therefore, UV-vis spectroscopy was used to investigate its coordinating behavior with CuCl2 ( Figure  2A). The UV-vis spectrum of polymer P1 exhibited a major absorption peak at around 231 nm and a minor one at around 291 nm. With the addition of CuCl2, the former peak gradually decreased, while the latter almost disappeared. More importantly, a new absorption peak appeared at around 270 nm, and its intensity constantly increased with the addition of CuCl2. The difference in UV-vis spectra indicates the change in the electronic environment of the nitrogen atoms and the new UV absorption band could be ascribed to the bonding σ(N) → antibonding dx2-y2(Cu) charge transfer (according to the literature), demonstrating the effective coordination between polymer P1 and the Cu 2+ ions [25,26]. Unexpectedly, polymer P1 emits blue fluorescence under UV light at 365 nm, even though it does not possess a conventional chromophore. Therefore, the excitation and emission spectra of P1 were studied to verify its fluorescent behavior. As illustrated in Figure 2B, the excitation wavelength appeared at 374 nm, and the emission wavelength appeared at 447 nm. This unconventional fluorescent phenomenon can be explained by the presence of N→Si coordination bonds in the polymeric backbones [27,28]. Photoluminescence would be generated by the through-space charge transfer from the lone electron pair in the nitrogen atoms to the 3d empty orbital of the silicon atoms. Moreover, the Unexpectedly, polymer P1 emits blue fluorescence under UV light at 365 nm, even though it does not possess a conventional chromophore. Therefore, the excitation and emission spectra of P1 were studied to verify its fluorescent behavior. As illustrated in Figure 2B, the excitation wavelength appeared at 374 nm, and the emission wavelength appeared at 447 nm. This unconventional fluorescent phenomenon can be explained by the presence of N→Si coordination bonds in the polymeric backbones [27,28]. Photoluminescence would be generated by the through-space charge transfer from the lone electron pair in the nitrogen atoms to the 3d empty orbital of the silicon atoms. Moreover, the N→Cu 2+ coordination interactions could lead to new charge transfer, thereby weakening the original N→Si coordination bonds, possibly inducing fluorescence quenching. To confirm this conjecture, fluorescent emission spectra were recorded after introducing Cu 2+ into the P1 solution in methanol. As shown in Figure 2C, the fluorescence emission intensity clearly decreased with the increase of the Cu 2+ content, indicating that this fluorescence quenching behavior was closely related to the N→Cu 2+ coordination property of polymer P1.

Hydrogen-Bonded and Metal-Coordinated Elastomers
Since there are hydrogen-bonding interactions between hydroxyl groups and between hydroxyl groups and nitrogen atoms in polymer P1, it is expected that these interactions might behave as physical crosslinking points to provide hydrogen-bonded elastomers. In addition, introducing strong metal coordination bonds into the weak hydrogen bonding network would lead to hierarchical non-covalent bond networks, allowing the flexible adjustment of elastomer properties. Upon deformation, weak hydrogen bonds tend to effectively dissipate energy by dynamic association and disassociation, while the strong coordination bonds can maintain high tensile strength. Therefore, a series of P1 elastomers with various contents of CuCl 2 were prepared.
According to the stress-strain curves shown in Figure 3A, the P1 elastomer showed the tensile strength of 0.70 MPa and the elongation at break of 490%, demonstrating the effective hydrogen-bonded crosslinking. Then various amounts of CuCl 2 were introduced into the P1 network to yield dually supramolecular elastomers named as P1-Cu-x/1, where the molar ratio of CuCl 2 vs. nitrogen atoms in P1 was 1/x. Upon adding 1/6 eq. CuCl 2 (vs. nitrogen atoms) to the polymer network, the tensile stress of the P1-Cu-6/1 sample was greatly increased up to 1.59 MPa, with the decrease of elongation at break to 337%, indicating the formation of a more compact network with higher crosslinking density resulting from the metal coordination. The mechanical properties of these elastomers varied greatly with the CuCl 2 molar ratios. When the amount of CuCl 2 increased to 1/4 eq., the tensile stress of the elastomer P1-Cu-4-1 reached 2.41 MPa, and the maximum tensile strain reached 287%. With an increase of CuCl 2 to 1/3 eq., the large number of CuCl 2 ions led to a heavily cross-linked polymer network. As a result, the P1-Cu-3-1 sample showed a tensile stress as high as 2.52 MPa, but the tensile strain decreased significantly to 268%. Meanwhile, the introduction of CuCl 2 also substantially increased the toughness and Young's modulus (E) of the elastomers. Among them, the P1-Cu-3-1 elastomer showed the highest toughness of 4.52 MJ/m 3 and E of 4.69 MPa. These results demonstrate that the mechanical properties of these elastomers can be flexibly adjusted by tuning the N/CuCl 2 molar ratio in the polymer network.  In addition to the mechanical properties, the thermal properties of the obtained elastomers were also significantly affected by the Cu/N coordination. Due to the adequate flexibility of the siloxane backbones, the hydrogen-bonded elastomer P1 possesses a low glass transition temperature (Tg) value ; however, the introduction of Cu 2+ can increase the degree of the crosslinking obtained elastomers, thus leading to the restriction of chain motion and hence, the increase of its Tg. The DSC results in Figure 3B showed that the Tg of P1 was found at −21.93 °C, whereas those of the metal-coordinated elastomers P1-Cu-6/1, P1-Cu-4/1 and P1-Cu-3/1 were measured at −17.43 °C, −14.08 °C, and −12.12 °C, respectively. In addition to hydrogen bonding, the presence of coordination in the P1-Cu samples was believed to decrease the mobility of the polymer chains, therefore increasing the Tg values. Meanwhile, no crystalline formation was observed for any elastomer under the studied experimental conditions, likely due to the poor crystallization ability of poly- In addition to the mechanical properties, the thermal properties of the obtained elastomers were also significantly affected by the Cu/N coordination. Due to the adequate flexibility of the siloxane backbones, the hydrogen-bonded elastomer P1 possesses a low glass transition temperature (T g ) value; however, the introduction of Cu 2+ can increase the degree of the crosslinking obtained elastomers, thus leading to the restriction of chain motion and hence, the increase of its T g . The DSC results in Figure 3B showed that the T g of P1 was found at −21.93 • C, whereas those of the metal-coordinated elastomers P1-Cu-6/1, P1-Cu-4/1 and P1-Cu-3/1 were measured at −17.43 • C, −14.08 • C, and −12.12 • C, respectively. In addition to hydrogen bonding, the presence of coordination in the P1-Cu samples was believed to decrease the mobility of the polymer chains, therefore increasing the T g values. Meanwhile, no crystalline formation was observed for any elastomer under the studied experimental conditions, likely due to the poor crystallization ability of polymer P1.
To demonstrate the coordination between the nitrogen atoms and copper ions in the P1-Cu elastomers, narrow XPS analysis using a high resolution was applied to measure the change in binding energy after adding CuCl 2 to the hydrogen-bonded elastomer. For P1-Cu-3/1, Figure 3C revealed that both the binding energy and intensity in the N 1S region were greater than those of P1. Furthermore, there was a shoulder peak at 934.0 eV for Cu 2p 3/2 peaks ( Figure 3D), which could be attributed to the Cu/N coordination complex, and the shake-up peaks at 939.9-943.9 eV and at 962.8 eV indicated the presence of partly coordinated Cu 2+ [29,30]. The charging of the electron cloud environments of the N and Cu atoms indicated that the lone pair electrons of the nitrogen atoms transferred to the empty orbitals of Cu 2+ ions, contributing to the physical crosslinking of the obtained elastomers.
The surface morphology holds important theoretical and practical significance for elastomers; therefore, the surface topographies of P1 and P1-Cu-3/1 were observed via SEM. Figure 4A,B showed that the introduction of coordination bonds did not affect the morphology of elastomers. A continuous and uniform surface morphology was observed, with no evidence of microphase separation, holes, or aggregation. This demonstrated that the coordination bonding between the poly(β-hydroxyl amine) matrix and metal ions was considerably strong, and high compatibility was observed inside the elastomers [31]. In addition, the element mapping obtained by EDS indicated that copper was successfully introduced into the supramolecular network and evenly distributed within the elastomer, similar to silicon ( Figure 4C,D).

Dynamic Properties of the Supramolecular Elastomers
Considering the reversibility of the hydrogen bonds and coordination bonds, along with the excellent flexibility of polymer P1, both the hydrogen-bonded elastomer P1 and the metal-coordinated P1-Cu are expected to possess self-healing capabilities. To prove this hypothesis, the P1 or P1-Cu-6/1 specimen was cut in half using a blade. The obtained cut-off pieces were then rejoined at the fracture surfaces and incubated at either room temperature (RT) or 60 °C for different durations. Figure 5A clearly showed that the ruptured surface was completely healed, withstanding the tensile stress. The typical tensile stress-strain curves of the pristine and healed P1 and P1-Cu-6/1 elastomers are shown in Figure 5B,D, respectively. Their self-healing efficiency is defined as the ratio of the tensile strength of the healed sample to that of the pristine sample.
After being held at RT for 48 h, the tensile strength and the strain at break of elastomer P1 were 0.38 MPa and 340%, respectively. As expected, the healing efficiency increased with the incubation time, manifested by 83% of tensile strength recovered after 96 h ( Figure 5C). Heating was more effective in increasing the self-healing efficiency, which reached up to 98% at 60 °C for 48 h. Nearly complete recovery of the original tensile curve was observed in Figure 3B, demonstrating the excellent self-healing capability of P1. In contrast, the healing efficiency of P1-Cu-6/1 decreased to 94% under the same conditions ( Figure 5E) because the higher crosslinking degree led to a greater restriction of segmental

Dynamic Properties of the Supramolecular Elastomers
Considering the reversibility of the hydrogen bonds and coordination bonds, along with the excellent flexibility of polymer P1, both the hydrogen-bonded elastomer P1 and the metal-coordinated P1-Cu are expected to possess self-healing capabilities. To prove this hypothesis, the P1 or P1-Cu-6/1 specimen was cut in half using a blade. The obtained cut-off pieces were then rejoined at the fracture surfaces and incubated at either room temperature (RT) or 60 • C for different durations. Figure 5A clearly showed that the ruptured surface was completely healed, withstanding the tensile stress. The typical tensile stress-strain curves of the pristine and healed P1 and P1-Cu-6/1 elastomers are shown in Figure 5B,D, respectively. Their self-healing efficiency is defined as the ratio of the tensile strength of the healed sample to that of the pristine sample.
After being held at RT for 48 h, the tensile strength and the strain at break of elastomer P1 were 0.38 MPa and 340%, respectively. As expected, the healing efficiency increased with the incubation time, manifested by 83% of tensile strength recovered after 96 h ( Figure 5C). Heating was more effective in increasing the self-healing efficiency, which reached up to 98% at 60 • C for 48 h. Nearly complete recovery of the original tensile curve was observed in Figure 3B, demonstrating the excellent self-healing capability of P1. In contrast, the healing efficiency of P1-Cu-6/1 decreased to 94% under the same conditions ( Figure 5E) because the higher crosslinking degree led to a greater restriction of segmental movement. In addition to self-healing abilities, both P1 and P1-Cu elastomers also exhibit excellent reprocessability, benefiting from the reversibility of the supramolecular interactions. For the reprocessing experiment, we placed the P1 elastomer pieces in a steel mold and then pressed it at 50 °C under 4 MPa for 20 min. After cooling to room temperature, the obtained film was cut into dumbbell-shaped samples and subjected to tensile tests to evaluate its mechanical properties ( Figure 6A). As shown in Figure 6B, the tensile properties of reprocessed-P1 were found to be nearly the same as those of the original P1, illustrating its excellent reprocessability. Meanwhile, although the metal coordination reduced the mobility, or flexibility, of the main chains, the networks containing metal ions still displayed favorable reprocessing properties. For example, after hot-pressing, the σmax and εb of P1-Cu-6/1 were found to be 1.58 MPa and 334%, respectively ( Figure 6C), which were nearly identical to the original values (1.59 MPa, 337%). In addition to self-healing abilities, both P1 and P1-Cu elastomers also exhibit excellent reprocessability, benefiting from the reversibility of the supramolecular interactions. For the reprocessing experiment, we placed the P1 elastomer pieces in a steel mold and then pressed it at 50 • C under 4 MPa for 20 min. After cooling to room temperature, the obtained film was cut into dumbbell-shaped samples and subjected to tensile tests to evaluate its mechanical properties ( Figure 6A). As shown in Figure 6B, the tensile properties of reprocessed-P1 were found to be nearly the same as those of the original P1, illustrating its excellent reprocessability. Meanwhile, although the metal coordination reduced the mobility, or flexibility, of the main chains, the networks containing metal ions still displayed favorable reprocessing properties. For example, after hot-pressing, the σ max and ε b of P1-Cu-6/1 were found to be 1.58 MPa and 334%, respectively ( Figure 6C

Applications for Photoluminescent and Conductive Supramolecular Elastomers
Given the integration of robust mechanical strength, superior extensibility, and excellent self-healing capability, both types of supramolecular elastomers show promising potential for use in photoluminescent materials and flexible electronic devices, such as strain sensors.
Lanthanide ions have a long-lived excited state and strong narrow-width emission bands in the visible region resulting from their f-f transitions [31,32]. Therefore, they are widely used in the preparation of photoluminescent materials such as fluorescent tubes, lasers, field-emission displays, and optical amplifiers. In this study, supramolecular elastomers P1-Eu with a photoluminescence capacity were successfully prepared based on the coordination of Eu 3+ ions with the polymer P1. Different amounts of Eu(NO3)3·6H2O were introduced into the P1 network to obtain photoluminescent supramolecular elastomers named P1-Eu-x, where the molar ratio of Eu(NO3)3·6H2O vs. nitrogen atoms in P1 was x.
Their solid-state fluorescent spectra were measured at the excitation wavelength of 365 nm. As shown in Figure 7A, the three elastomers P1-Eu-4%, P1-Eu-10%, and P1-Eu-20% all exhibited the characteristic emission peaks of Eu 3+ ions at 591 nm and 617 nm. The former peak was assigned to the 5D0→7F1 transition of the Eu 3+ ions, while the latter resulted from the 5D0→7F2 transition. The emission intensities at 591 and 617 nm varied with the N/Eu 3+ ratios. In addition, the very strong emission peak at 617 nm illustrated the highly polarized chemical environment of the Eu 3+ ions. As demonstrated above, the P1 elastomer itself would also exhibit the emission at 443 nm under the excitation of 365 nm. Therefore, the photoluminescent colors of the P1-Eu samples resulted from both the Eu 3+ ions and the P1 elastomers. As shown in Figure 7B, the emission color change could be easily observed in the CIE-1931 RGB coordinates, which were calculated from the emission spectra. As the Eu 3+ content increased, these materials showed a continuous color change from blue to cyan, and finally, to bright green.

Applications for Photoluminescent and Conductive Supramolecular Elastomers
Given the integration of robust mechanical strength, superior extensibility, and excellent self-healing capability, both types of supramolecular elastomers show promising potential for use in photoluminescent materials and flexible electronic devices, such as strain sensors.
Lanthanide ions have a long-lived excited state and strong narrow-width emission bands in the visible region resulting from their f-f transitions [31,32]. Therefore, they are widely used in the preparation of photoluminescent materials such as fluorescent tubes, lasers, field-emission displays, and optical amplifiers. In this study, supramolecular elastomers P1-Eu with a photoluminescence capacity were successfully prepared based on the coordination of Eu 3+ ions with the polymer P1. Different amounts of Eu(NO 3 ) 3 ·6H 2 O were introduced into the P1 network to obtain photoluminescent supramolecular elastomers named P1-Eu-x, where the molar ratio of Eu(NO 3 ) 3 ·6H 2 O vs. nitrogen atoms in P1 was x.
Their solid-state fluorescent spectra were measured at the excitation wavelength of 365 nm. As shown in Figure 7A, the three elastomers P1-Eu-4%, P1-Eu-10%, and P1-Eu-20% all exhibited the characteristic emission peaks of Eu 3+ ions at 591 nm and 617 nm. The former peak was assigned to the 5D 0 →7F 1 transition of the Eu 3+ ions, while the latter resulted from the 5D 0 →7F 2 transition. The emission intensities at 591 and 617 nm varied with the N/Eu 3+ ratios. In addition, the very strong emission peak at 617 nm illustrated the highly polarized chemical environment of the Eu 3+ ions. As demonstrated above, the P1 elastomer itself would also exhibit the emission at 443 nm under the excitation of 365 nm. Therefore, the photoluminescent colors of the P1-Eu samples resulted from both the Eu 3+ ions and the P1 elastomers. As shown in Figure 7B, the emission color change could be easily observed in the CIE-1931 RGB coordinates, which were calculated from the emission spectra. As the Eu 3+ content increased, these materials showed a continuous color change from blue to cyan, and finally, to bright green.
Another potential application of elastomer P1, that is, for use in the production of self-healable electronic devices, was further investigated. A self-healing conductive elastomer, P1-MWCNT, was successfully prepared via the combination of hydrogen-bonded elastomer P1 and multiwalled carbon nanotubes (MWCNT) ( Figure 8A; σ max = 1.39 MPa, ε b = 231%). To qualitatively evaluate the electrical conductivity of the P1-MWCNT elastomer, a closed circuit consisting of a piece of P1-MWCNT (20 × 8 × 0.7 mm 3 ), a small LED bulb, a regulated power supply (7 V), and some connecting wires was designed. As shown in Figure 8B, the LED lamp was instantly illuminated by switching on the power supply. When the sample was subjected to a tensile strain of approximately 50%, the luminous intensity of the LED lamp dropped correspondingly. When the elastomer was cut in half using a blade, the LED light immediately turned off. However, after the two cut surfaces made contact and self-healed, the LED lamp was again illuminated. Similarly, as the repaired elastomer continued to be stretched, the brightness of the LED lamp decreased due to the increase in resistance. Another potential application of elastomer P1, that is, for use in the production of self-healable electronic devices, was further investigated. A self-healing conductive elastomer, P1-MWCNT, was successfully prepared via the combination of hydrogen-bonded elastomer P1 and multiwalled carbon nanotubes (MWCNT) ( Figure 8A; σmax = 1.39 MPa, εb = 231%). To qualitatively evaluate the electrical conductivity of the P1-MWCNT elastomer, a closed circuit consisting of a piece of P1-MWCNT (20 × 8 × 0.7 mm 3 ), a small LED bulb, a regulated power supply (7 V), and some connecting wires was designed. As shown in Figure 8B, the LED lamp was instantly illuminated by switching on the power supply. When the sample was subjected to a tensile strain of approximately 50%, the luminous intensity of the LED lamp dropped correspondingly. When the elastomer was cut in half using a blade, the LED light immediately turned off. However, after the two cut surfaces made contact and self-healed, the LED lamp was again illuminated. Similarly, as the repaired elastomer continued to be stretched, the brightness of the LED lamp decreased due to the increase in resistance.   Another potential application of elastomer P1, that is, for use in the production of self-healable electronic devices, was further investigated. A self-healing conductive elastomer, P1-MWCNT, was successfully prepared via the combination of hydrogen-bonded elastomer P1 and multiwalled carbon nanotubes (MWCNT) ( Figure 8A; σmax = 1.39 MPa, εb = 231%). To qualitatively evaluate the electrical conductivity of the P1-MWCNT elastomer, a closed circuit consisting of a piece of P1-MWCNT (20 × 8 × 0.7 mm 3 ), a small LED bulb, a regulated power supply (7 V), and some connecting wires was designed. As shown in Figure 8B, the LED lamp was instantly illuminated by switching on the power supply. When the sample was subjected to a tensile strain of approximately 50%, the luminous intensity of the LED lamp dropped correspondingly. When the elastomer was cut in half using a blade, the LED light immediately turned off. However, after the two cut surfaces made contact and self-healed, the LED lamp was again illuminated. Similarly, as the repaired elastomer continued to be stretched, the brightness of the LED lamp decreased due to the increase in resistance.  Next, to preliminary explore the response behavior of the P1-MWCNT to external strain, a piece of P1-MWCNT with an initial size of 20 × 8 × 0.4 mm 3 was subjected to various strains to determine the change in resistance as ∆R/R 0 ; ∆R and R 0 refer to the resistance variation upon stretching and the initial resistance, respectively. Figure 8C reveals that the measured resistance value gradually increased with the increase in deformation. When the P1-MWCNT was stretched 225%, its ∆R/R 0 value reached 410%. It was believed that the tight MWCNT would gradually become loose during the stretching process, which would destroy the conductive path and increased the resistance. According to the above results, it is reasonable to conclude that this supramolecular elastomer shows promising potential for future use in flexible strain sensors.

Conclusions
In summary, we have demonstrated that silicon-containing poly(β-hydroxyl amine)s synthesized via the polymerization between 1,3-bis(3-glycidyloxypropyl)tetramethyldisiloxane and 3-amino-1,2-propanediol are value building blocks for preparing stretchable, selfhealable, and reprocessable supramolecular elastomers. Among the obtained elastomers, the hydrogen-bonded elastomer exhibits an unconventional fluorescence behavior owing to the unique Si-N coordination and displays a low T g value resulting from the sufficient flexibility of the siloxane main chains. The mechanical properties of the metal-coordinated elastomers can be flexibly adjusted by varying the molar ratio of N/CuCl 2 . Moreover, these elastomers show excellent self-healing properties and hot-pressing reprocessability. Notably, we also prepared photoluminescence-tunable materials and self-healing conductive elastomers by combining the elastomers with Eu 3+ and MWCNT, respectively. Considering the facile accessibility, adjusted mechanical properties, and outstanding dynamic capacities, these novel supramolecular elastomers based on poly(β-hydroxyl amine)s could find application for use as sustainable materials, fluorescent materials, and flexible electronic sensors.