Haruka Takebuchi and
Ren-Hua Jin*
Department of Material and Life Chemistry, Kanagawa University, 3-2-7 Rokkakubashi, Yokohama 221-8686, Japan. E-mail: rhjin@kanagwa-u.ac.jp
First published on 15th February 2022
Photoluminescent polymers can be divided into two types of structures: one is the well-known conventional π-conjugated rigid chain polymers bearing π-conjugated chromophores in their side chains, and the other is the common flexible polymers without π-conjugated chromophores in their main or side chains but with a feature of clustering electron-rich and/or dipole groups in their main and/or side chains. In this work, we found a new photoluminescent polymer comprising theophylline (T) and imidazole (I) residues in a suitable ratio in the side chains on the common polystyrenic block (PVB-T/I). We synthesized a block copolymer (denoted as P2) consisting of hydrophobic PVB-T/I and hydrophilic poly(N-isopropylacrylamide), and we investigated its self-assembly into micelles and their micellar features, such as thermo-responsibility, fluorescence emission, pH, and metal ion-dependent photoluminescence, in detail. Especially, the micelles self-assembled from P2 showed intrinsic blue emission which was emitted from the charge transfer association between T and I residues in the intra-chains. Weakening the association by adjustment of the pH or addition of metal ions could evidently reduce the photoluminescence in the micellar state. Very interestingly, among many metal cations, only Pd2+, which can chelate strongly with theophylline, strongly quenched the photoluminescence from the micelles. Therefore, the polymer micelles functioned as an optical sensor for Pd(II) ion not only by spectroscopy but also with the naked eye.
There are many reports about luminescent polymers with π-conjugated moieties24–31 such as pyrene,24,25 porphyrin,26 and rhodamine27,28 in their side chains and/or end groups. Although these luminescent polymers have high potential for sensors, fluorescence probes and imaging materials, they possess poor hydrophilicity and/or readily cause aggregation quenching. Therefore, they are not good candidates for use in the aggregated state in aqueous systems. As a useful tool for adapting photofunctional polymers to aqueous media, the polymers are often constructed as amphiphiles possessing hydrophobic luminescent segments and hydrophilic moieties, by which it is feasible to respond not only to light but also to environmental changes such as heat and pH.32–39 These designed polymers can enhance the effect of the luminescence emission and thus make it possible to control the ON/OFF switching of their sensing power, which exerts its function in a certain environment. For example, introducing some moieties with the property of aggregation-induced emission (AIE) in the hydrophobic block could enhance the fluorescence emission of the amphiphilic block copolymer in aqueous media due to the appearance of self-assembled entities driven by hydrophobic interactions between the AIE moieties.40 Different from such AIE systems, in the case of aggregation-caused quenching (ACQ), π-conjugated polymers such as poly[fluorenyl-alt-p-phenyleneethynylene] (PFPE) backbones with pendant carboxylic acid groups can function very well as fluorescent sensors for distinguishing aliphatic and aromatic amines in aqueous media; aliphatic amines associated with pendant groups of carboxylic acid cause extension of the π-conjugated polymer chains to overcome ACQ, while aromatic amines interact with the π-conjugated polymer chains with π–π interactions, forcing ACQ.31
In the issue of π-conjugated polymers, the imidazole-conjugated structure is also very effective for developing photoluminescent materials.41 Imidazole is a heterocyclic compound with an imine group as a proton acceptor and an amine group as a proton donor in the same aromatic ring, and imidazole itself is also sensitive to pH and/or metal ions. The architecture of π-conjugated polymers containing imidazole rings or imidazole-condensed rings has attracted much attention because of their photonic properties as charge transfer chromophores and the unique photophysical process of excited-state intramolecular proton transfer (ESIPT).42–44 Imidazole-conjugated polymers bearing proton-donating phenol side groups can cause effective ESIPT by photoexcitation when they form intramolecular hydrogen bonds between the imidazole and phenol groups.45 In this system, however, the covalent conjugation between the electron donor and electron acceptor (often an imidazole moiety) is indispensable. Although there are remarkable achievements of polymers possessing imidazole-condensed rings as side chains on their photoactive main chains, such as polythiophene and polycabazole, it is rare that luminescent polymers contain imidazole rings but possess no π-conjugation backbone structures.
Recently, nonconventional fluorescent polymers without π-conjugation structures have also drawn great research interest.46–48 Among them, water-soluble hyperbranched polyethyleneimine (h-PEI) is especially interesting. Luo and coworkers reported that h-PEI reacted with aldehydes could function as light emission polymers due to the formation of Schiff base bonds.49–51 In this hyperbranched structure, the Schiff base bonds could crowd into clusters which are very similar to AIE to increase the radiative decay when excited.50,51 They also demonstrated that the emission of the Schiff base bond-based h-PEI could respond to pH or acidic compounds and metal ions in aqueous media.49 In practice, many polymers, even those without conventional chromophores (only have groups of cyano, imine, carbonyl, tertiary amine, etc.), are also potentially photoluminescent materials, as the polymers afford definite aggregates through which space conjugation occurs.52 Polyacrylonitrile is a typical nonconventional chromophore which can emit blue fluorescence in the solid state when excited by UV light.53
Very recently, we revealed that theophylline, an imidazole-condensed xanthine derivative, is a strong receptor of Pd(II) ions due to the formation of an extraordinary stable complex with Pd(II), and we found that polymers bearing residues of the theophylline coordinated-Pd(II) complex could function as good catalysts in C–C coupling reactions.54,55 Herein, we focused our attention on multiple stimuli-responsive issues in the design of an amphiphilic block copolymer comprising a pH/photo-responsive non-conjugated hydrophobic polystyrenic block with pendant rings of a xanthine derivative (theophylline) and imidazole and a thermo-responsive hydrophilic block of PNIPAM. We firstly synthesized a block copolymer that consisted of a poly(vinylbenzyl chloride) (PVBC) block and PNIPAM block via RAFT polymerization, and then we introduced theophylline (xanthine derivative) and/or imidazole pendants into the PVBC block. By changing the ratio of theophylline (T) and imidazole (I) in the pendants, we prepared targeting polymers of PVB(T/I)-b-PNIPAM, where T/I was altered to 100/0, 77/23 and 0/100. It was found that PVBT-b-PNIPAM (P1, T/I = 100/0) and PVBT/I-b-PNIPAM (P2, T/I = 77/23) appeared to be amphiphiles that could easily form micelles in aqueous media, while PVBI-b-PNIPAM (P3, T/I = 0/100) became a double-hydrophilic block copolymer which dissolved in water. All the polymers showed thermo-responding ability due to possessing a PNIPAM block. Very interestingly, polymer P2 with T/I in a definite ratio in its side groups showed remarkably blue emission, although P1 and P3 themselves are weakly or not emissive under the same conditions. We revealed that intra-polymer chain associations between theophylline and imidazole in the side chains of P2 functioned as an intricate emitter to afford blue emission. This emitter acted as an excellent optical sensor for Pd(II) ion because Pd ion strongly chelates with the theophylline moiety, resulting in dissociation of the emitter and thus in quenching of the photoluminescence.
Imidazole and theophylline dissolved in chloroform showed absorption peaks at 241 nm and at 273 nm, respectively (Fig. S5†). With this as a reference, we measured the UV-Vis absorption of polymers P0–P3. As shown in Fig. 2A, there are no absorption peaks at 273 nm for P0 or P3, which contain no theophylline moiety. In contrast, P1 and P2 showed absorption at 273 nm due to the presence of theophylline residues in the pendant. In the expansion of the spectral line from 300 to 400 nm (Fig. 2A′), we can see that P3 with only imidazole in its pendants gives a tailing line, while P2, which contains both imidazole and theophylline in its side chains, exhibits an obvious shoulder at around 340 nm, although P1 has no absorption in this area.
Fig. 2 (A) UV-vis spectra of PVB(T/I)-b-PNIPAM in CHCl3 measured at 25 °C. (B) is the enlarged area around 300–400 nm of (A). The polymer concentration is 2 g L−1. |
To understand the thermophysical properties of the polymers, we performed differential scanning calorimetry (DSC) measurements for the block copolymers of P0–P3 (Fig. 3A) and the homopolymers of PVBC74, PVBT74 and PNIPAM334. As can be seen from Fig. 3B, the glass transition temperatures (Tg) for the homopolymers of PVBC74 and PNIPAM334 appeared at 89.2 °C and 124.8 °C, respectively. After the introduction of theophylline into PVBC74, the corresponding PVBT74 showed a Tg of 180.3 °C, indicating that the pendant theophylline makes the polymer chains rigid and enhances the interactions between the polymer chains. In comparison, the block copolymers P0–P3, which consisted of PNIPAM383 and polystyrenic blocks possessing different side chains, showed similar Tg values of around 141–145 °C, which are higher than the Tg values of the homopolymers PVBC74 and PNIPAM334 but lower than the Tg of the homopolymer PVBT74. It seems that there is no formation of individual phases from the two blocks of polystyrenic derivatives (with smaller DP 74) and PNIPAM (with larger DP 383). Probably, the good compatibility between the two blocks enhances the miscibility of the polymer chains, leading to a homogeneous phase with a new glass transition temperature (Tg).
Since the block copolymers possess longer PNIPAM blocks, they should exhibit thermo-responsibility in aqueous media. Therefore, we conducted micellar dispersions of P1 and P2 and the solution of P3 in a thermo-heater-equipped DLS and UV-Vis spectrometer to investigate the thermo-responsivity of the polymers in aqueous media. At room temperature, the P1 and P2 dispersions showed hydrodynamic diameters of 89 and 71 nm, respectively, indicating the formation of polymeric micelles, while the P3 solution did not show a light scattering signal because of the molecular solution (see Fig. 4A). As shown in Fig. 4B, when the dispersions were heated to 45 °C, the hydrodynamic diameter increased to 380 nm for P1 but decreased to 24 nm for P2. In comparison, at 45 °C, heating-triggered micellization occurred from the molecular solution of P3 due to dehydration of the PNIPAM block, showing a hydrodynamic diameter of 200 nm. On the other hand, at a wavelength of 500 nm, we compared the temperature-dependent transparences of the samples. As can be seen from Fig. 4C, below 30 °C, the transparence of the dispersion of P1 was over 30%, but it decreased to near zero as the temperature increased to 35 °C. The transparence of the P3 dispersion decreased from 92% to 50% as it was heated to 50 °C, and the micelles of P2 only showed a slight change from 87% to 77% even when heated to 50 °C. This change is in agreement with the heat-induced change of the micellar size. The smaller the micellar size, the higher the transparency, and the larger the micellar size, the lower the transparency. Apparently, each polymer that possessed the PNIPAM block indicated an LCST but at different temperatures. The LCSTs for P1, P2 and P3 appeared at 30 °C, 30 °C and 34 °C, respectively. Here, the relationship between the transmittance and heating/cooling cycles for the micellar dispersion of P1 were conducted in the temperature range between 25 °C and 45 °C with 10 min intervals. As shown in Fig. 4D, the thermo-response is highly reversible in each recycle. P2 and P3 also responded well with reversibility on heating and cooling recycles (data not shown). The thermo-response of P1 was also confirmed by 1H NMR spectroscopy in D2O (see Fig. S6†). At 25 °C, only the peaks due to the isopropyl group of PNIPAM appeared. This is because of the formation of core–shell micelles in which the polystyrenic block with theophylline pendants formed a core (non-solvated solid state) while the PNIPAM block formed a shell layer (solvated coil state). When heated to 45 °C, the peaks due to the chemical shifts of PNIPAM disappeared, indicating the phase-transition of the PNIPAM shell into dehydrated globules from hydrated coils. Photographs of the samples in vials at room temperature and under heated conditions are displayed in Fig. S7.† The solutions of P1 and P3 became remarkably opaque, while that of P2 did not show distinguishable cloudiness. These findings are also in agreement with the argument based on the results shown in Fig. 4.
Based on the above results, the thermo-responsivity of the micellar dispersions can be explained as illustrated in Fig. 5. Below the LCST, P1 exists as core–shell micelles with a PVBT core and PNIPAM shell. Above the LCST, the shell of the micelles from P1 loses water due to dehydration of PNIPAM, and some inter-micellar interactions take place to form larger micellar aggregates. This is reversible with heating and cooling. Similarly, P2 forms core–shell micelles below the LCST. However, the micelles of P2 do not associate with each other above the LCST but form smaller micelles. This should arise from the contributions of intra-micellar interactions: that is, the shrinking of the PNIPAM shell leads the PNIPAM chains to collapse onto the micellar core and enhances the intra-micellar polymer-to-polymer interactions between PNIAPM and the theophylline/imidazole moieties existing in the core surface. Compared to P1, the thermo-response of P2 micelles is restricted only to intra-micelle contact. It seems that the pathway of thermo-response towards inter-micellar or intra-micellar is determined by the core components; the core gathered with theophylline alone causes inter-micellar association of the shells, while the core consisting of random arrangements of theophylline/imidazole leads only to intra-micellar collapse. In contrast to both the amphiphilic polymers of P1 and P2, the double hydrophilic block copolymer P3 is a unimer coil below the LCST but becomes core–shell micelles with the formation of the PNIPAM core and PVBI shell above the LCST.
Fig. 5 Schematic of the self-assembly of the temperature-responsive PVB(T/I)-b-PNIPAM series in water. |
Fig. 6 Fluorescence emission spectra (λex = 365 nm) of the micellar and unimer solutions of P1–P3 (2 g L−1) at room temperature (A) and at 45 °C (B). |
In the above emission spectrum measurements, the amounts of the two residues of T and I in P2 solution (2 mL of 2 g L−1) are equal to 3.4 mmol and 1.0 mmol, respectively. Therefore, we prepared a solution containing P1 (only theophylline pendants) and P3 (only imidazole pendants) with a ratio of T/I of 77/23 (in molar) and subjected the solution to fluorescence measurements to confirm whether the mixture could function as an emitter similar to P2. As shown in Fig. S8D,† it is obvious that there is no enhancement of the emission from the mixture. We also performed comparative fluorescence measurements by using two aqueous solutions; one contained monomeric theophylline and imidazole in a molar ratio of 77/23 (3.4 mmol (0.60 mg)/1.0 mmol (0.07 mg) in 2 mL water), [T] + [I] = 0.22 mmol mL−1, and the other was a mixture of imidazole with P1 micelles with a ratio of T/I of 77/23. In both cases, however, no fluorescence increment appeared (Fig. S8B and C†). These results indicate that the emission could not be strengthened from the mixtures containing theophylline and imidazole residues either as low molecular state or as polymeric pendants in the given conditions. Only P2, which has random copolymeric structures containing theophylline and imidazole in a suitable ratio in its pendants, emits fluorescence strongly at low concentration. Accordingly, the appearance of remarkable emission from P2 should be assigned to the synergy effect of the intramolecular (intra-chain) interactions between the moieties of theophylline and imidazole in the pendants, which are crowded in one polymer chain. As a derivative of xanthine, the ring in the theophylline plane condensed with imidazole would be more electron-poor than the imidazole ring itself. Therefore, the imidazole plane could act as an electronic donor to interact with the theophylline plane via π–π interactions to form charge-transfer-like associates. The appearance of a shoulder around 340 nm in the UV-Vis spectrum of P2 (Fig. 2B) could be related to the associates caused by π–π interactions. From the excitation spectrum of the micellar dispersion of P2 (Fig. S8A†), we observed that P2 showed a remarkable absorption peak at 365 nm, which is a maximum excitation wavelength, either in the aqueous micellar state or in chloroform solution. This excitation peak should be attributed to emitters that may be charge transfer (or excimer- and exiplex-like) associates in the clusters of theophylline and imidazole residues introduced densely in the polymer side chains. In these associates, the bond of imine –CN– in theophylline or imidazole is basic and is thus able to function as a proton acceptor and/or ligand to metal cations. Therefore, we expect that the fluorescence emission from the associates could respond to pH and/or metal cations because the imine –CN– is capable of accepting protons or of chelating with metal cations.49
Here, we prepared P2 micelles at different pH values by adding a DMSO solution of P2 to excess water pH-adjusted in advance with HCl or ammonia solution, and then we examined their fluorescence emissions. As shown in Fig. 7A, the emission intensity is the same in the cases of pH 7.0 and 10.2 but became very weak at pH 2.2. This unambiguously indicates that the forces supporting the emitters formed via π–π interactions from theophylline and imidazole residues are weakened due to competitive interactions arising from protonation of the imine bond –CN–. We also compared the diameters of the micelles prepared in the different pH conditions. In Fig. 7B, it can be seen that the micellar diameters become larger by nearly ten times (278 nm) in the acidic conditions (pH 2.2) compared to the neutral (33 nm) and basic (25 nm) conditions. It needs to be noted here that the emission and diameter of the micelles did not change as the pH was lowered to 4 from 7. However, as the pH values changed in the order of 3.2, 2.9 and 2.7, the micellar sizes and the fluorescence emissions increased and decreased, respectively, in a stepwise fashion (see Fig. S9†). We think that during the formation of core–shell micelles, the protonated –NC– bonds in the hydrophobic block weaken the hydrophobic and π–π interactions between the hydrophobic blocks and thus cause the core sediment to lack close packing, resulting in core-loose micelles with larger diameters. The thermo- and excitation-responsibility were also examined for the pH-adjusted P2 micelles. As shown in Fig. S10A,† the light transparence at a wavelength of 500 nm is very low (about 15%) for the micelles formed at pH 2.2 but high (about 90%) for the micelles formed at both pH 7.0 and 10.2 at 25 °C. As they were heated, the micelles formed at pH 2.2 turned opaque at 31 °C, while the transparence decreased slightly to 74% at 38 °C for the micelles formed at pH 7.0 and to 84% at 36 °C for the micelles formed at pH 10.2. This means that the smaller micelles formed at the higher pH values showed higher LCSTs than the lager micelles formed at lower pH, although the PNIPAM homopolymer itself has no pH-related thermo-response. In addition, in the excitation spectra of the micelles, the absorption at the maximum excitation wavelength is lower for the micelles formed at pH 2.2 than for the micelles formed at pH 7.0 and 10.2 (see Fig. S10B†), which is in agreement with the fluorescence emission response to pH changes (see Fig. 7A). Therefore, it is conclusive that amphiphilic P2 randomly bearing theophylline/imidazole in the side chains on the hydrophobic block is a unique photoluminescent polymer with thermo- and pH-responses, although it contains no π-conjugated polymeric chains. The photoluminescence should arise from the charge-transfer-like π–π association between imidazole and theophylline in adjacent spaces in which clusters crowded by the basic imine bond –CN– would play a central role in the emission.49,52 Once the imine –CN– is protonated, the π–π associations of the theophylline and imidazole residues will be disturbed, and thus the photoluminescence will be reduced. As far as we know, this is a new insight into the architecture of photoluminescent polymers comprising imidazole analogous residues but without rigid imidazole-conjugated polymeric chains. These photoluminescent polymers would have very interesting potential in optical-mediated response to metal ions because the basic –CN– prefers chelation interactions with metal cations and not only with protons.
Fig. 8 Bottom: Fluorescence emission spectra (λex = 365 nm) of micellar dispersions of P2 (2 g L−1) in the presence of 2.5 mM metal acetate at room temperature. Top: photographs of the dispersions. |
In order to further confirm the sensing behavior of P2 micelles, we performed post-addition of Pd2+ cations to a micellar dispersion. In Fig. S12,† the photographs and SEM images are displayed. Compared to the case of P2/Pd2+ micelles formed by simultaneous mixing of P2 and Pd2+ cations, upon the post-addition of Pd2+ cations (2.5 mM), the P2 micelles rapidly became turbid, with the formation of orange sediment (Fig. S12A†). This color suggests the formation of a Pd(II)/theophylline complex which shows absorption at wavelengths around 400–500 nm.55 The sediments visualized by SEM are fibrous network entities which are likely formed by linking of the fibrously fused micelles. Perhaps, the post-added Pd2+ cations chelate with the theophylline and imidazole residues which exist on the core surface and thus promote one-dimensional growth of inter-micellar fusion but do not destroy the micelles. In comparison, when the concentration of the post-added Pd2+ cation was as low as 0.025 mM (5.6 ppm), the P2 micelles remained stable without sediments (Fig. S12B†), accompanying a noticeable reduction of the photoluminescence intensity to 9%. This indicates that Pd2+ cations at a lower concentration chelate with theophylline/imidazole residues via intra-micellar interactions and thus effectively quench the emission (Fig. S12C†). As a comparison, using the opaque mixture of P1 + P3 (T/I = 7/3, 2 g L−1), we performed a similar experiment, as shown in Fig. S13 and 14,† in the presence of Pd cations at 0.25 and 0.025 mM. The emission from the mixture decreased only slightly (about 20%) when Pd2+ cations were added at 0.025 mM, while it decreased almost completely when the concentration of Pd2+ cations added was increased to 0.25 mM, although there was no precipitation. The ability of P2 was well beyond that of the mixture of P1 and P2 to sense a low concentration of Pd2+ cations.
To confirm the selective palladium sensing, we further performed the examination of the photoluminescence of P2 in the case of co-existence of several metal cations. As shown in Fig. 9A, the emission intensity of P2 was reduced to 44% in the co-presence of three ions of Ag+, Zn2+ and Cu2+. Comparatively, in the case of the co-presence of four ions of Pd2+, Ag+, Zn2+ and Cu2+, the emission intensity was reduced greatly to 8.7%, indicating high selectivity of P2 for Pd2+ cations over other metal cations. This quenching effect is equal to the case of Pd2+ cations only. Without a doubt, even when Pd2+ cations are mixed with other metal cations such as Ag+, Zn2+, and Cu2+, the emission quenching is selectively induced by the palladium cations by excluding the other metal cations from moving close to P2. From the photographs in Fig. 9B, it can be seen clearly that the two micellar dispersions coexisting with several metal cations remained in the micellar state without sediments. Under UV light irradiation, the micellar dispersion containing Ag+, Zn2+, and Cu2+ still emits noticeable blue light, while the micellar dispersion in which Pd2+ was added to Ag+, Zn2+, and Cu2+ barely showed the original blue. This suggests that the sensing of Pd2+ cation by P2 can be judged even with the naked eye.
There are many reports of the sensing of Pd2+ cations depending on an optical process using organic fluorescent compounds that can turn their emission “ON” or “OFF” when they chelate with Pd2+ cations.58–65 However, the synthesis of the special fluorescent compounds is expensive. Our polymer reported here with common theophylline and imidazole moieties is not only inexpensive but also simply and effectively useable as an optical sensor for palladium cations.
PVBC74-CDB (1.00 g, equal to 87.1 μmol of CDB end groups), AIBN (4.3 mg, 26 μmol), N-isopropylacrylamide (NIPAM) (9.84 g, 87.1 mmol) and 1,4-dioxane (16.3 g, 60 wt%) were mixed in a Schlenk tube. After the solution was degassed by three freeze–pump–thaw cycles, the sample tube was heated at 65 °C for 6 hours. Then, the crude product diluted with THF was precipitated three times in n-hexane and dried at 40 °C in vacuo. Yield: 4.3 g. GPC: Mn = 60022, Mw = 75649, PDI: 1.260, DP = 383.
The procedure of removal of thiocarbonylthio end-groups from the above diblock copolymer was as follows. A 100 mL round-bottomed flask was charged with PVBC74-b-PNIPAM383-CDB (2.0 g, 37 μmol of CDB end groups, Mn (NMR) = 55 kg mol−1), BPO (0.177 g, 0.73 mmol), and 1,4-dioxane (60 mL). The solution was refluxed for 1 hour at 80 °C under nitrogen atmosphere to remove the end-groups of dithiobenzoate. The crude product was diluted with THF, precipitated in a large amount of n-hexane 4 times and then dried under vacuum. Yield: 1.8 g. GPC: Mn = 61177, Mw = 98649, PDI = 1.61.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra08756h |
This journal is © The Royal Society of Chemistry 2022 |