Zengfang Huang*ab,
Yali Chenab,
Runze Wangab,
Chaoyue Zhouab,
Xiaobo Liub,
Liucheng Maoc,
Jinying Yuanc,
Lei Taoc and
Yen Wei*c
aSchool of Materials & Food Engineering, Zhongshan Institute, University of Electronic Science & Technology of China, Zhongshan, 528402, P. R. China. E-mail: hzf105@163.com
bSchool of Materials and Energy, University of Electronic Science & Technology of China, Chengdu, 610054, P. R. China
cDepartment of Chemistry, The Tsinghua Center for Frontier Polymer Research, Tsinghua University, Beijing 100084, P. R. China. E-mail: weiyen@tsinghua.edu.cn
First published on 4th February 2020
Recently, AIE-active fluorescent materials have attracted extensive investigation due to their significant applications in the fields of memory devices, photomodulation, information displays, sensors, and biological imaging. In this contribution, a novel acrylate AIE-active dye of TPMA was successfully synthesized by Suzuki coupling and acylation reaction, and belongs to the monoclinic crystal system and P21/c space group from the crystal structure analysis, and its fluorescence intensity was stronger with an obvious red shift of emission wavelength as compared with the reported TPB dye. Moreover, the obtained TPMA dye exhibits multi-stimuli-responsivity and a two-photon fluorescent switch with excellent reversibility in the solid state. Subsequently, the corresponding fluorescent polymers of PEG-TM were successfully fabricated via RAFT polymerization of TPMA and PEGMA with a molecular weight of about 25000 (Mn) and narrow polydispersity index (PDI). From 1H NMR analysis, when the feeding ratio of TPMA increased to 32.2% from 19.2%, the molar fraction of TPMA in PEG-TM polymers accordingly increased to 32.8% from 19.5%. In water solution, the as-prepared PEG-TM1 polymers would self-assemble into fluorescent organic nanoparticles (FONs) with diameters ranging from 150 to 250 nm, and their maximum emission wavelength presented at 518 nm with obvious AIE phenomena. Moreover, the as-synthesized PEG-TM polymers have prospective application in biological imaging due to their good fluorescence, high water solubility and excellent biocompatibility.
As one of the effective polymerization methods, reversible addition-fragmentation chain transfer (RAFT) polymerization has developed into the most famous and widely used technology in synthesis chemistry and polymer chemistry due to its simple operation, mild reaction conditions, many applicable solvent and wide range of monomers.23–25 The obtained polymers by RAFT polymerization have the characteristics of controlled molecular weight, narrow molecular weight distribution and precise structure. Therefore, RAFT polymerization is considered to be an important and effective way to prepare multifunctional copolymers, which is widely used in materials science, biology, electronics, etc.26–32 For example, amphiphilic block copolymer p(HEMA-b-Azo-IEM) was successfully prepared by RAFT polymerization, in water solution, which self-assembled into micelles, and its size and shape changed with the different light irradiation (visible/UV light).33 Phenylboronic acid derivatives have been widely used in the synthesis of glucose-sensitive materials in the field of biomedicine due to their specific interaction with biological molecules such as glucose and glycoproteins. Nanogels p(AAPBA-AGA-BODIPYMA) were synthesized by RAFT polymerization, the fluorescence intensity and size of which were sensitive to glucose. Meanwhile, the nanogels had good compatibility, and could encapsulate and release insulin, indicating that the nanogels had the potential to detect glucose and treat diabetes.34 A cross-linked copolymer (PEG-co-FHMA) was constructed by RAFT polymerization with hydrazine hydrate as cross-linking agent. The as-prepared copolymer had excellent AIE property, good fluorescence, low critical micelle concentration and good biocompatibility, which make it a powerful candidate for bioimaging.35
Stimuli-responsive fluorescence switching by molecular assemblies transformation with external stimuli is attracting considerable interest due to its significant applications in memory devices, photomodulation, information displays, and sensors. Due to the excellent fluorescence and easy modification of TPE together with mild reaction conditions and many suitable monomers of RAFT polymerization, in this study, we try our best to fabricate novel TPE polymers with AIE-activity by RAFT polymerization. Firstly, a novel methacrylate functionalized-TPE TPMA dye was synthesized with multi-stimuli-responsivity and two-photon fluorescent switch with excellent reversibility in the solid state, which was very favorable for cells imaging due to the strong fluorescence intensity and obvious red shift of emission wavelength as compared with the reported TPB dye. Subsequently, the corresponding polymers PEG-TM were successfully synthesized via RAFT polymerization combining the hydrophilic monomer PEGMA with the various feeding ratio of TPMA. The amphiphilic PEG-TM polymers would self-assemble into FONs in water, which exhibited the prospective application in bioimaging due to the good fluorescence performance, high water solubility and excellent biocompatibility.
The average molecular weight (Mn) and polydispersity index (PDI) of the polymer PEG-TM were analyzed by a Waters 1515 gel permeation chromatography (GPC) system with a refractive index detector taking tetrahydrofuran (THF) as the eluent. The 1H NMR spectra of TPEOM, TPEOH, fluorescent monomer TPMA and fluorescent polymers PEG-TM was characterized by a JEOL JNM-ECA 400 (400 mHz) spectrometer with tetramethylsilane (TMS) as a reference. Transmission electron microscopy (TEM) images were measured on a JEM-1200EX high resolution electron microscope at a working voltage of 100 kV, in which the PEG-TM suspension were previously dropped onto carbon-coated copper grids and then naturally dried. FT-IR spectral data was measured on a PerkinElmer Spectrum 100 spectrometer (Waltham, MA, USA), in which the KBr method and the reflection mode were respectively adopted depending on the status of the sample. UV-Vis absorption spectrum was measured on a PerkinElmer LAMBDA 35 UV/Vis spectroscopy system. The fluorescence emission and excitation spectra were measured on a PE LS-55 spectrometer. Single crystal X-ray diffraction data of the TPMA dye were measured on a Bruker Smart CCD diffractometer and its structure was solved by Patterson methods followed by different Fourier syntheses and then refined by full-matrix least squares techniques against F2 with SHELXTL.39
The ORTEP diagram of complex TPMA dye is presented in Fig. 1(A), which belongs to monoclinic crystal system and P21/c space group. a = 29.6191(12) Å, b = 5.7006(2) Å, c = 17.6543(6) Å, α = 90°, β = 100.620(4) °, γ = 90°, V = 2929.81(19) Å3, Z = 4, R1 = 0.0702, wR2 = 0.1357. The dihedral angle between the benzene rings of C3–C4–C5–C6–C7–C8 and C9–C10–C11–C12–C13–C14 is about 87.460°, and the dihedral angle between the benzene rings of C15–C16–C17–C18–C19–C20 and C21–C22–C23–C24–C25–C26 is about 89.551°, indicating the angulation structure of the phenyl rings owing to the steric effect of TPE segment. Otherwise, the dihedral angle between the benzene rings of C21–C22–C23–C24–C25–C26 and C30–C31–C32–C33–C34–C35 is about 8.934°, and they are almost in the same plane, which endows TPMA dye the good conjugative effect. The bond length of C(27)–C(28) was between the C–C single bond and CC double bond length due to its conjugation with phenyl rings of C21–C22–C23–C24–C25–C26 and C30–C31–C32–C33–C34–C35. From the bond length analysis, the bonds of O(1)–C(33) and O(2)–C(36) were respectively single bond and double bond, indicating the successful demethylation reaction of –OCH3 and acylation reaction of –OH. Fig. 1(B) showed the calculated HOMO and LUMO spatial distributions and optimized structure in the ground states of TPMA dye by the Gaussian 09 program which was carried out at the B3LYP/6-31G* level. The electrons of TPMA at HOMO were mainly located at the tetraphenylethene segment, while most of the electrons transferred to the diphenyl rings with cyano group at the LUMO, and the calculated transition energy ΔE of HOMO and LUMO was about 5.27 eV.
The synthesized PEG-TM1 polymers had an average molecular weight (Mn) of about 25000 g mol−1 and its polydispersity index (PDI) is about 1.30, as shown in Fig. 2(A), and the Mn of PEG-TM2 polymers was about 27000 g mol−1. The similar Mn of them should originate from two factors, one hand, the higher Mn of TPMA should increase the Mn of PEG-TM2 polymers as compared with PEGMA; on the other hand, the steric effect of TPMA possibly affect the chain propagation rate to a certain degree. The 1H NMR spectra of TPEOM, TPEOH, TPMA and fluorescent polymers PEG-TM were shown in Fig. 2(B). From the 1H NMR spectrum of TPEOM, a single peak at 3.84 ppm could be clearly observed, which belonged to the characteristic proton peak of –CH3, indicating that the 4-methoxyphenylacetonitrile was introduced into the molecular structure by the expected condensation reaction. By comparing and analyzing the TPEOH spectrum with the TPEOM spectrum, the characteristic proton peak of –OH appeared at 4.91 ppm in the spectrum of TPEOH, while the single peak of 3.84 ppm completely disappeared, which indicated that the methoxy group of TPEOM was completely reacted out and successfully converted to a hydroxyl group by demethylation reaction. For the fluorescent monomer TPMA, the two characteristic proton peak of –CCH2 appeared at 5.56 ppm and 6.11 ppm, indicating the desirable introduction of methacryloyl group by acylation reaction of –OH and methacryloyl chloride. According to the analysis of the spectra of the polymers PEG-TM1 and PEG-TM2, after the RAFT polymerization, the characteristic proton peak of –CCH2 in the monomer of TPMA was completely disappeared. Moreover, the aromatic ring peaks of TPMA obviously appeared at 7.04–7.68 ppm. Another characteristic peaks located at 4.08 ppm could be assigned to the ester groups of poly-(PEG). Combining the analysis results of the above 1H NMR spectra, it can be concluded that all reactions proceed as expected as shown in the schematic diagram, and the desired fluorescent monomer TPMA and fluorescent polymers are obtained. It is generally known that the peak area of 1H NMR spectra is directly proportional to the corresponding number of characteristic hydrogens. Therefore, the actual molar ratio of TPMA in PEG-TM polymers was further analyzed by calculating the integral ratio of the characteristic peaks of 7.04–7.68 ppm and 4.08 ppm. The results showed that the molar ratio of TPMA increased to 32.8% in PEG-TM2 from 19.5% in PEG-TM1 while the feeding molar fraction of TPMA increased to 32.2% from 19.2%.
Fig. 2 (A) The GPC trace of PEG-TM1 (THF) (Mn = 25000, PDI = 1.30); (B) 1H NMR spectra (CDCl3) of TPEOM, TPEOH, fluorescent monomer TPMA and fluorescent polymers PEG-TM. |
Fig. 3 showed the results of further studies on the RAFT polymerization kinetics of TPMA and PEGMA. According to the analysis of the 1H NMR spectra of Fig. 3(A), the peaks at 5.60 ppm and 6.15 ppm were attributed to the –CCH2 proton peaks of PEGMA, and the peaks at 5.81 ppm and 6.39 ppm were attributed to the –CCH2 proton peaks of TPMA. The conversion of PEGMA and TPMA can be calculated from the intensity change of –CCH2 with a characteristic peak at 6.80 ppm of trimethylbenzene as the internal standard. From the Fig. 3(A), the intensity of the peaks at 6.15 ppm and 6.39 ppm gradually decreased as the reaction progressed, which meant that PEGMA and TPMA had been gradually consumed by the RAFT polymerization to successfully construct the PEG-TM polymers. After 36 hours of polymerization, two monomers reached high conversion rates. The kinetic study showed a linear pseudo-first-order kinetic curve as a function of time, as shown in Fig. 3(B). In the early stage of polymerization, the conversion of TPMA was significantly higher than that of PEGMA, so the molar fraction of TPMA in the polymers gradually increased. With the progress of polymerization, the conversion of TPMA almost remained unchanged and the conversion of PEGMA gradually increased, which would result in a gradual decrease in the molar fraction of TPMA in the polymers and a gradual increase in the molar fraction of PEGMA because the concentration of TPMA in the reaction mixture was less and less as compared with that of PEGMA, in other words, the obtained PEG-TM polymers were nearly gradient polymers.
As compared with previously reported TPB dye, the fluorescence intensity of TPMA significantly increased with the red shift of the maximum emission wavelength. As shown in Fig. S1,† the emission wavelength of TPMA increased to 500 nm with a marked increase of fluorescence intensity, while the emission wavelength of TPB dye was 470 nm with the very weak fluorescence intensity under the same condition. The increase of the fluorescence emission wavelength of the dye could effectively enhance the light transmittance and reduce light damage, which meant that TPMA was more favorable for bioimaging. As an electron-withdrawing group, the –CN group would average the electron cloud distribution of the dye TPMA with additional conjugation effect, thereby reducing the energy transition from the first excited state S1 to the ground state S0, which resulted in the red shift of fluorescence emission.40 The fluorescence emission spectrum of the TPMA dye in the solid state was further measured, and its maximum emission wavelength appeared at 483 nm, accompanied by strong blue-green light observed under ultraviolet light. Surprisingly, when the sample was ground, the color of the TPMA dye changed from light yellow to bright yellow, and the maximum emission wavelength was red-shifted to 526 nm with strong green light observed under ultraviolet light, as shown in Fig. 4. Then the ground sample was annealed, the maximum emission wavelength of TPMA was changed from 526 nm back to 483 nm. Repeated grinding and annealing of the samples gave similar results, confirming that TPMA had good reversibility between the two wavelengths, which should attribute to the transformation of TPMA between amorphous and crystalline structures.41 Aside from annealing, solvent–vapor-induced crystallized samples (S1v, S2v and S3v) are obtained from the ground samples. The good reversibility between the two wavelengths is similar with the above phenomenon, suggesting that both annealing and vapor inducement can promptly revert high two-photon fluorescence from green light to blue light with multi-stimuli-responsivity.
According to the results of 1H NMR analysis, it can be firmly determined that the two monomers of TPMA and PEGMA polymerized to form the polymers PEG-TM, in other words, the polymers PEG-TM simultaneously contained hydrophobic segments and hydrophilic segments, so that the polymers PEG-TM had amphiphilicity property. The different affinity of hydrophobic and hydrophilic segments with water could cause microphase separation, which made the amphiphilic polymers PEG-TM exhibit self-assembly property in water. The hydrophobic TPMA fragments gathered together spontaneously, while the hydrophilic PEGMA fragments autonomously wrapped around the periphery of the TPMA aggregates to form nanoparticles with orderly assembled core–shell structures. In order to verify the successful self-assembly of polymers in water, their structure and morphology were studied by transmission electron microscopy (TEM). Spherical particles with a diameter in the range of 150 to 250 nm can be clearly observed from Fig. 5(A), which was the result of the successful self-assembly of the amphiphilic polymer PEG-TM1 in water. This result also proved the success of RAFT polymerization from the side. In order to corroborate the results of 1H NMR analysis, the structure of TPEOM, TPEOH, TPMA and PEG-TM1 were better study and their FT-IR spectra were illustrated in Fig. 5(B). From the spectrum of TPEOM, the stretching vibration peak of –CN bond could be easily found at 2230 cm−1, which meant that the 4-methoxyphenylacetonitrile was introduced into the molecular structure. As compared with the spectrum of TPEOM, the spectrum of TPEOH presented another sharp peak at 3320 cm−1, which could be considered as the stretching vibration of O–H, demonstrating that boron tribromide successfully translated the methoxy group of TPEOM into a hydroxyl group of TPEOH. For the fluorescent monomer TPE-MA, the peak at 3320 cm−1 completely disappeared, and a new typical absorption peak appeared at 1720 cm−1, which corresponded to the stretching vibration of CO. Further, the peak at 2950 cm−1 was related to the stretching vibration motion of C–H on the alkane chain, which completely confirmed that TPEOH was successfully subjected to an acylation reaction with methacryloyl chloride to introduce a methacryloyl group. From the spectrum of the polymer PEG-TM1, three obvious representative absorption peaks were noticed, which were respectively located at 2880, 1720 and 1100 cm−1, being closely related to the stretching vibrations of –CH2–, CO and C–O. In summary, the spectrum of PEG-TM1 simultaneously showed the characteristic structure of TPMA and PEGMA, which further proved that TPMA and PEGMA were successfully introduced into the polymers PEG-TM1 through RAFT polymerization.
The amphiphilic polymers PEG-TM would exhibit self-assembly characteristic in water due to the microphase separation caused by different affinity of TPMA and PEGMA segments with water. In water, the amphiphilic polymer PEG-TM1 self-assembled into the corresponding FONs, and their UV-visible absorption spectrum was shown in Fig. 5(C). There were three distinct absorption peaks at 248, 309 and 370 nm, respectively. The peak at 248 nm was closely related to the π → π* electronic transition of polycyclic aromatic hydrocarbons. Meanwhile, the molecular structure of the polymers contained heteroatoms O and N, whose n → π* electronic transition of lone pair electrons caused absorption peaks at 309 nm and 370 nm. When the wavelength was greater than 450 nm, the absorbance was almost zero which was not affected by light scattering and Mie effect, suggesting that the PEG-TM1 polymers had high water solubility and dispersion in water.42,43 The fluorescence spectra of the PEG-TM1 polymers in water and THF were shown in Fig. 5(D). In water, the maximum emission wavelength of PEG-TM1 presented at 518 nm with strong green luminescence, while in THF there was almost no fluorescence, indicating that PEG-TM1 had obvious AIE characteristic. In a good solvent such as THF, the intramolecular rotation of PEG-TM1 polymer was spontaneous and active. When PEG-TM1 was stimulated by external energy ultraviolet light, they would absorb external energy and transited to the excited state from the ground state S0. Then the unstable molecules would return to the S0 from the excited state through the active intramolecular motion, which was an effective non-radiative pathway for the attenuation of the excited state energy. When the PEG-TM1 polymer self-assembled into nanoparticles in water, the hydrophobic TPMA fragments would aggregate inside the PEG-TM1 FONs, and the interaction of the various molecules limited their intramolecular rotation, thus the excited state energy attenuated through the radiation pathway, inducing the fluorescence emission.
Then the possibility of PEG-TM1 FONs in cell imaging applications were further explored by confocal laser scanning microscope (CLSM).50,51 Under the irradiation of 405 nm laser, as shown in Fig. 6(B)–(D), the CLSM images of L929 cells were taken which were nurtured with 20 μg mL−1 PEG-TM1 FONs for 3 hours. The treated L929 cells showed an obvious green fluorescence, which was consistent with the fluorescence emitted by the PEG-TM1 FONs, indicating that PEG-TM1 FONs have been taken up by the cells through endocytosis. At the same time, it could be observed that each cell contained a region with very weak fluorescence. A comprehensive comparison of the size differences of PEG-TM1 FONs and various organelles in the cells determined that the region with very weak fluorescence was identified as the nucleus, which also indicated that PEG-TM1 FONs mainly concentrated in the cytoplasm region after being taken up by the cells. Based on all the characterization and experimental results, PEG-TM1 FONs have good fluorescence property, high water dispersibility and good biocompatibility. Moreover, PEG-TM1 FONs showed good imaging effects after entering into the cells by endocytosis, indicating that the prepared PEG-TM1 FONs were a good bioimaging material with broad application prospects.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 1910007. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c9ra10430e |
This journal is © The Royal Society of Chemistry 2020 |