Although the role of extracellular Ca2+ draws increasing attention as a messenger in intercellular communications, there is currently no tool available for imaging Ca2+ dynamics in extracellular regions. Here we report the first solid-state fluorescent Ca2+ sensor that fulfills the essential requirements for realizing extracellular Ca2+ imaging. Inspired by natural extracellular Ca2+-sensing receptors, we designed a particular type of chemically-crosslinked polyacrylic acid gel, which can undergo single-chain aggregation in the presence of Ca2+. By attaching aggregation-induced emission luminogen to the polyacrylic acid as a pendant, the conformational state of the main chain at a given Ca2+ concentration is successfully translated into fluorescence property. The Ca2+ sensor has a millimolar-order apparent dissociation constant compatible with extracellular Ca2+ concentrations, and exhibits sufficient dynamic range and excellent selectivity in the presence of physiological concentrations of biologically relevant ions, thus enabling monitoring of submillimolar fluctuations of Ca2+ in flowing analytes containing millimolar Ca2+ concentrations.
Ca2+ plays a crucial role in many important physiological and pathological processes in animals1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17 and plants9,18,19,20,21,22,23. Over the past several decades, many synthetic molecular and genetically encoded fluorescent Ca2+ indicators have been developed, as represented by 1,2-bis(o-aminophenoxy)-ethane-N,N,N′,N′-tetraacetic acid (BAPTA) derivatives24,25,26,27 and calmodulin-based proteins28,29,30,31,32, respectively. Ca2+-imaging techniques that use such fluorescent indicators are indispensable in modern biology and medical science. In living organisms, Ca2+ concentrations differ greatly depending on the compartment. Typically, the Ca2+ concentration is ~100 nanomolar (nM) in intracellular cytosol, ~100 micromolar (μM) in the endoplasmic reticulum and mitochondria and ~1 millimolar (mM) in extracellular fluid and blood (Fig. 1a,b)3. Plant vacuoles are also considered to contain mM-order Ca2+ concentrations20. Hence, Ca2+ imaging in all of these compartments requires dedicated fluorescent indicators with specific dissociation constants (Kd) that are appropriate for the respective background Ca2+ concentrations. However, almost every Ca2+ indicator known to date has a Kd value ranging from nM to μM, and therefore allows for Ca2+ imaging only in cytosol and organelles (Fig. 1a). Fluorescent Ca2+ indicators with mM-order Kd, compatible with extracellular Ca2+ concentrations27,32, have scarcely been developed9,10, despite the fact that extracellular Ca2+, which is conventionally regarded as a diagnostic indicator for many diseases3,7, is now receiving considerable attention as a first messenger3,4,5,6,7,8,9,10,11,12,13,14,15,16,17 in, for example, parathyroid gland3,4, neuron12,13, myocyte14, stem cell15 and macrophages16,17.
In fact, there are major problems in the development of indicators for extracellular Ca2+ imaging9,10. First, such indicators should be designed to strike a balance between mM-order Kd (i.e., a rather small affinity for Ca2+) and high selectivity for Ca2+ in the presence of excessive amounts of other physiological ions. Although simple Ca2+ imaging against mM-order background concentration of Ca2+ may be possible using existing indicators with μM-order Kd, Ca2+ indicators with one-order higher Kd have a great advantage in monitoring Ca2+ transients and oscillations in extracellular regions. Even more challenging in extracellular Ca2+ imaging, one has to create a mechanism to avoid the outflow of indicators from an observation area through molecular diffusion. Obviously, this issue is intractable with existing molecular-based indicators.
Here we report a conceptually new fluorescent Ca2+ sensor that can clear up all the above problems. It is a solid-state (gel) sensor that consists of a chemically-crosslinked polyacrylic acid (PAA), and its sensing mechanism relies not on conventional host-guest chemistry using tailored Ca2+-binding sites but on polymer-chain dynamics triggered by Ca2+. We show that ordinary PAA, when given pendants of tetraphenylethene (TPE), an aggregation-induced emission (AIE) luminogen33,34,35, becomes fluorescent in the presence of Ca2+. This series of polymers (PAA-TPEx, Fig. 1c) has mM-order apparent Kd for Ca2+ and can selectively sense Ca2+ against high background concentrations of physiological ions, glucose and amino acids. Remarkably, its chemically-crosslinked gel (g-PAA-TPEx, Fig. 1c,d) inherits the excellent Ca2+ selectivity and mM-order Kd of PAA-TPEx, thus providing a solid-state sensor that enables not only spatial imaging of Ca2+ in a macroscopic biological sample such as brain slices but also temporal detection of submillimolar fluctuations (±0.2 mM) in the Ca2+ concentration in a flowing analyte containing ~1 mM Ca2+.
Results and Discussion
As a clue for the design of the new sensor, we took notice of CaSR, a natural extracellular Ca2+-sensing receptor4,6, which senses the change of Ca2+ concentration in extracellular regions and sends a signal to intracellular regions (Fig. 1b). Unlike calmodulin36,37, CaSR does not have particular high-affinity Ca2+-binding amino acid sequences4,6 and instead possesses highly acidic domains containing clusters of carboxylic acid functionalities (Fig. 1b). The acidic domains are believed to be responsible for Ca2+ binding. This holds true for the extracellular Ca2+-sensing receptor (CAS) in plants21 as well as other low-affinity Ca2+-binding proteins38,39. Regarding the interaction between Ca2+ and clustering carboxylic acid domains in CaSR and CAS, we found an interesting analogy with a work of Flory40, which had shown that the intrinsic viscosity of PAA in water decreases considerably upon addition of Ca2+ (25–50 mM). Subsequent reports, including those of Ikegami et al.41 and Huber et al.42,43, have indicated that mM-order Ca2+ causes the single-chain aggregation of PAA in water, for which [CO2−–Ca2+–−O2C]-type ion binding is responsible44. Importantly, among major ions in the body (Na+, K+, Mg2+ and Ca2+), Ca2+ most effectively triggers such conformational change of the PAA chain40,41,42,43.
Inspired by the analogy between natural and synthetic polymers, we designed PAA-TPEx with an expectation that the conformational change of PAA chain between aggregation and expansion upon binding and release of Ca2+, respectively, might be translated into the fluorescence property of the TPE pendants (Fig. 1e). AIE luminogens, in contrast to usual fluorescent dyes, are known to fluoresce upon aggregation and are only weakly fluorescent in the molecularly dispersed state33,34,35. We also conceived that, if such a polymer-based indicator could be properly crosslinked, the resultant gel (a macroscopic material) might serve as a solid-state Ca2+ sensor with mM-order Kd, which allows for long-term monitoring of extracellular Ca2+ dynamics at the organ level.
Random copolymers PAA-TPEx (Fig. 1c, Table 1, entries 1–5) containing 1–5 mol% (x = 0.01–0.05) of TPE pendants were synthesized by a two-step procedure involving the free-radical copolymerization of TPE-appended acrylate 1 and t-butyl acrylate 2 with the corresponding feed ratio (1/2 = 1/99–5/95) and the subsequent removal of t-butyl groups from the resulting copolymers using trifluoroacetic acid (Fig. 2, see Methods for details). The chemical structure of PAA-TPEx was unambiguously characterized by nuclear magnetic resonance (NMR) and infrared (IR) spectroscopy (Supplementary Figs S20 and S21). By means of gel permeation chromatography (GPC) using polystyrene standards, we estimated the number mean molecular weight (Mn) of PAA-TPEx to be approximately 20 kDa (Table 1, entries 1–5).
Although PAA-TPEx (10 mg/L) in a buffer solution ([4-(2-hydroxyethyl)-1-piperazineethanesulfonic acid (HEPES)] = 70 mM, pH = 7.4) scarcely fluoresces, it becomes fluorescent upon addition of CaCl2. For example, the fluorescence intensity of PAA-TPE0.02 increased monotonically as the Ca2+ concentration was increased from 0.01 to 10 mM (Fig. 3a). As shown in the Ca2+ titration curves (Fig. 3b), the increase in fluorescence intensity occurred regardless of the TPE content (x = 0.01–0.05) (Table 1, entries 1–5). When PAA-TPEx loses Ca2+, its polymer chain returns to a weakly fluorescent random-coil state. As soon as ethylenediaminetetraacetate (EDTA), a strong chelator for Ca2+ (Kd = ca. 10–10 M), was added to a buffer solution containing, e.g., PAA-TPE0.02 (10 mg/L) and Ca2+ (30 mM), the fluorescence was mostly quenched (Fig. 3a, green line). All of the above observations demonstrate that the Ca2+-triggered aggregation of the PAA chain is reflected in the fluorescence intensity of TPE. Notably, even PAA-TPE0.01, which has a TPE content of only 1 mol%, can successfully visualize the change in Ca2+ concentration. Dynamic light scattering (DLS) experiments confirmed that the increase in the fluorescence intensity of PAA-TPE0.02 is due to single-chain aggregation40,41,42,43 rather than interpolymer aggregation. As shown in Fig. 4a,b, when Ca2+ concentration was increased, the fluorescence intensity as well as the particle size (hydrodynamic diameter, Dh) of PAA-TPE0.02 increased (Fig. 4b,e). In contrast, on aging at 25 °C with a constant Ca2+ concentration (e.g., 0.4 mM), the particle size of PAA-TPE0.02 increased (Fig. 4c,d, blue symbols), while its fluorescence intensity remained almost unchanged (Fig. 4d, red symbols and Fig. 4e).
Fitting the Ca2+ titration curve (Fig. 3b and Supplementary Fig. S2a) using Hill’s equation provided the apparent Kd of PAA-TPEx for Ca2+ (see Methods for details). As shown in Table 1 (entries 1–5), the values were all on the order of mM and ranged from 0.43 to 2.8 mM depending on the TPE content (x). The apparent Kd decreased as the TPE content increased, suggesting that the hydrophobic nature of TPE promotes the Ca2+-triggered single-chain aggregation of PAA-TPEx. Importantly, because the relationship between the logarithm of the apparent Kd and the TPE content is approximately linear (Fig. 3c, blue symbols), the apparent Kd of PAA-TPEx can be continuously tuned in the range between 0.43 and 2.8 mM by simply varying the TPE content (x). This feature is beneficial for detecting a change in the Ca2+ concentration against various background concentrations of ions and provides an interesting contrast to typical molecular indicators such as the Fura series25, the Kd values of which are controlled by the electronic properties of the substituents on the BAPTA skeleton.
The single-chain aggregation of PAA-TPEx and in turn the enhancement of fluorescence intensity occurs very selectively for Ca2+. Without Ca2+, PAA-TPEx is weakly fluorescent in the presence of high concentrations of major ions in the body, i.e., Na+ (145 mM), K+ (5 mM) and Mg2+ (2 mM), as well as a physiological concentration (50 μM) of trace ions, i.e., Fe2+, Cu2+, Zn2+, Al3+, Sr2+ and Ba2+ (Fig. 3f and Supplementary Fig. S3a,b). Moreover, glucose (14 mM) and all the natural amino acids (5 mM) did not significantly influence the fluorescence property of PAA-TPEx (Fig. 3f and Supplementary Fig. S3a–d). To further test the selective sensing capability of PAA-TPEx, we performed a Ca2+ titration experiment using a buffer solution ([HEPES] = 70 mM, pH = 7.4) containing PAA-TPE0.02 (10 mg/L), Na+ (145 mM), K+ (5 mM), Mg2+ (2 mM), glucose (14 mM) and glutamine (5 mM). Upon addition of CaCl2, the fluorescence of the buffer solution of PAA-TPE0.02 intensified (Supplementary Fig. S4a). Note that PAA-TPEx can recognize Ca2+ selectively in the presence of such a high concentration of Mg2+ (Supplementary Figs S5 and S6). Based on the titration curve (Supplementary Fig. S4b), the apparent Kd and the dynamic range (ratio of the maximum to the minimum fluorescence intensity) were determined to be 9.2 mM and 25, respectively. The difference of the apparent Kd for Ca2+ in the presence (9.2 mM) and absence (1.8 mM) of the biologically relevant ions and sugar likely arises from competing interactions of the carboxyl group of PAA with other metal ions and/or the polar functionalities of glucose and amino acid. This trend is generally observed for existing Ca2+ indicators25. From Ca2+ titration experiments under different pH (e.g., pH = 7.0 and 8.1) and temperature (25–40 °C) conditions, we confirmed that such pH and temperature changes exert little influence on the Ca2+ sensing property of PAA-TPE0.02 (Supplementary Figs S7 and S8).
The mM-order Kd, excellent selectivity and sufficient dynamic range of PAA-TPEx for Ca2+ fulfill the essential requirements of sensing Ca2+ against high background concentrations of physiological ions. For the subsequent challenge in realizing a solid-state Ca2+ sensor, we prepared a chemically-crosslinked gel of PAA-TPEx. Typically, TPE-appended acrylate 1 (2 mol%) and acrylic acid 3 (95 mol%) were copolymerized in the presence of tetraethyleneglycol diacrylate 4 (3 mol%) as a crosslinker (Fig. 2, see Methods for details). The resultant gel (g-PAA-TPE0.02) was insoluble but swelled in aqueous media and could be readily processed into various shapes and sizes such as large-area flexible sheets and micro particles (Supplementary Fig. S9). When a droplet of a buffer solution of CaCl2 (30 mM) was placed on a large-area gel sheet, blue fluorescence emerged (Supplementary Movie S1), clearly demonstrating that PAA-TPE0.02, even when chemically crosslinked, can respond to Ca2+. The Ca2+-sensing property of g-PAA-TPE0.02 was largely dependent on the total monomer concentration in the copolymerization rather than the feed ratio of the crosslinker. We optimized the preparation conditions in terms of the total monomer concentration as well as the feed ratio of the crosslinker (Supplementary Fig. S10) so that the dynamic range could be maximized (Supplementary Fig. S11). The best results (dynamic range = 12) were obtained when the total monomer concentration was 1.5 M and the feed ratio of the crosslinker was 3 mol% (Supplementary Fig. S11a, entry 9 and Supplementary Fig. S11b, red block). We found that g-PAA-TPE0.02 thus obtained was the most swollen (Supplementary Fig. S11c, red symbol). Conversely, copolymerization at high total monomer concentrations (e.g., 4.0 M) resulted in a less-swollen gel that scarcely responded to Ca2+ (Supplementary Fig. S11a, entries 1–4, Supplementary Fig. S11b, blue blocks and Supplementary Fig. S11c, blue symbols). Because the degree of polymer-chain entanglement generally decreases when the total monomer concentration is decreased45, g-PAA-TPE0.02, obtained under the optimized conditions (Supplementary Fig. S11a, entry 9), may maintain the mobility of the polymer chains to a large extent and undergo conformational changes upon binding to Ca2+. Meanwhile, the change in the feed ratio of the crosslinker did not impact largely on the dynamic range and swelling ratio of g-PAA-TPE0.02 (Supplementary Fig. S11a, e.g., entries 1–4), indicating that the physical crosslinking due to polymer-chain entanglement is more important than the chemical crosslinking in determining the mobility of the polymer chain45 and in turn Ca2+-sensing properties of the gel.
At the optimal total monomer concentration (1.5 M), 1 and acrylic acid 3 were copolymerized with varying molar ratios (1/3 = 1/96–5/92) in the presence of tetraethyleneglycol diacrylate 4 (3 mol%). The resultant materials (g-PAA-TPEx, x = 0.01–0.05) were all swollen in aqueous media and capable of sensing Ca2+ selectively (Fig. 3f). Table 1 (entries 6–10) summarizes the apparent Kd and the dynamic range of g-PAA-TPEx as determined by titration experiments (Fig. 3d and Supplementary Fig. S2b). Importantly, each g-PAA-TPEx has an apparent Kd value comparable to that of the corresponding non-crosslinked PAA-TPEx. As in the case of PAA-TPEx, the logarithms of the apparent Kd values correlated linearly with the TPE contents of g-PAA-TPEx (x < 0.05, Fig. 3c, red symbols), indicating that the sensitivity of the gel sensor is tunable. The swelling ratios also correlated linearly with the TPE contents of g-PAA-TPEx (x < 0.05, Fig. 3c, green symbols). Consequently, the apparent Kd values were proportional to the swelling ratios (Fig. 3e). The TPE-content dependence of the apparent Kd and swelling ratio most likely originates from the hydrophobic nature of TPE. We presume that the hydrophobic TPE pendants pre-aggregate in the swollen gel even without Ca2+ to engage in crosslinking of the polymer chains non-covalently (i.e., pseudo crosslinking). Hence, high-level loading of the TPE pendant (x = 0.05) would result in a decrease in the degree of freedom of the polymer chains to decrease the dynamic range. In fact, less-swollen g-PAA-TPE0.05 exhibited the smallest dynamic range among g-PAA-TPEx (Table 1, entry 10).
g-PAA-TPEx could be used in various sizes and shapes (Supplementary Fig. S9). For example, a gel sheet fabricated from g-PAA-TPE0.02 allowed spatial visualization of the Ca2+-concentration distribution. A simple stamp experiment, using shaped filter papers impregnated with two aqueous solutions with different Ca2+ concentrations (Fig. 5a–d), demonstrated that the difference in the Ca2+ concentration can be distinguished with the naked eye as a difference in fluorescence intensity (Fig. 5d–f). A stamp experiment using biological samples may demonstrate the potential of the gel sensor in biomedical applications. In this context, we observed subtle fluorescence behavior of g-PAA-TPE0.02 in a titration experiment using an albumin protein (bovine serum albumin, BSA). At BSA concentrations below 1.0 g/L, the fluorescence intensity of the gel monotonically increased, and then gradually decreased, mostly recovering its initial value at a BSA concentration of 20 g/L (Supplementary Fig. S12a). At this stage, upon subsequent addition of Ca2+, the gel turned fluorescent again (Supplementary Fig. S12b). Although the origin of these observations is unclear, we found that the influence of the protein on the Ca2+-sensing property of the gel can be avoided by covering the gel surface with a dialysis membrane, which may prevent proteins from contacting the gel. For instance, when a mouse brain slice was put on a gel sheet of g-PAA-TPE0.02 through a dialysis membrane and then removed, brain-shaped fluorescence emerged on the gel sheet (Supplementary Fig. S13a,b,d). As a control experiment, when a mouse brain slice was immersed in an EDTA solution for removing Ca2+ and then likewise stamped on a gel sheet of g-PAA-TPE0.02, minimal fluorescence was observed from the gel (Supplementary Fig. S13c,d). In situ imaging with fluorescence microscopy successfully visualized the microscopic distribution of Ca2+ in the brain slice (Supplementary Fig. S14).
Using gel sheets immobilized on a vessel, the diffusion of Ca2+ in a buffer solution could be visualized spatiotemporally (Fig. 5g and Supplementary Movie S2). To further examine the feasibility of the stationary detection of a change in the Ca2+ concentration in a flowing analyte, we monitored fluorescence in a microtomed section of g-PAA-TPA0.02 immobilized in a microfluidic channel (Fig. 5h and Supplementary Figs S15 and S16). Traumatic events such as epileptic seizures and terminal anoxia are accompanied by 1 mM-level changes in the Ca2+ concentration in the extracellular fluid inside the brain46. For a model experiment, we prepared, as a pseudo extracellular fluid, two buffer solutions of a mixture of physiological ions ([Na+] = 145 mM, [K+] = 5 mM, [Mg2+] = 2 mM and [glucose] = 14 mM) containing 1.1 or 0.1 mM Ca2+. When these solutions were alternately flowed through the microfluidic channel with the gel, reversible changes in fluorescence intensity were observed in response to changes in the Ca2+ concentration (Fig. 5i). More surprisingly, the gel recognized a small fluctuation (±0.2 mM) of the Ca2+ concentration against high background concentrations of physiological ions. Figure 5j shows serially repeated changes in fluorescence intensity under the alternating flow of pseudo extracellular fluids containing 1.1 or 1.3 mM Ca2+. Such a submillimolar fluctuation in the Ca2+ concentration is known to be associated with normal brain activity47. This result demonstrates the great potential of g-PAA-TPEx as a tool for realizing extracellular Ca2+ imaging.
We have demonstrated that conventional polyacrylic acid (PAA), when an aggregation-induced emission luminogen is attached to its main chain, provides a state-of-the-art solid-state fluorescent Ca2+ sensor, which can selectively detect submillimolar fluctuations of Ca2+ concentration. The fact that acidic domains with clustering carboxylic acid groups exist ubiquitously in natural extracellular Ca2+-sensing receptors as well as low-affinity Ca2+-binding proteins inspired us to use ordinary PAA that has been long known to undergo single-chain aggregation in the presence of mM-order Ca2+. The gel sensor is easy to synthesize at a large scale (Fig. 1d), has high processability (Supplementary Fig. S9), and can exert its superb function at high Ca2+ concentration even in the presence of competing amounts of alkali, alkaline-earth metal ions, sugars and amino acids. Considering its high potential, the gel sensor may serve as the first imaging tool for investigating the hitherto unexplored field of fluorescence extracellular Ca2+ imaging, eventually leading to comprehensive understanding of biological events involving Ca2+, particularly at the macroscopic organ levels. Besides the biological applications, the present sensor may be used in more general fields such as food and environmental inspection25,49.
Unless otherwise noted, all the commercial reagents were used as received. Prior to use, t-butyl acrylate (2), acrylic acid (3), tetraethylene glycol diacrylate (4), 1,4-butanediol diacrylate (7) and 1,10-decanediol diacrylate (8) were purified by passage through Al2O3 column to remove polymerization inhibitors. Azobisisobutyronitrile (AIBN) and N,N′-methylenebis-acrylamide (6) were purified by recrystallization from methanol. 4-(1,2,2-triphenylvinyl)phenol (5) was prepared according to the reported procedure50.
(See Fig. 2).
4-(1,2,2-triphenylvinyl)phenyl acrylate (1)
A CHCl3 (5 mL) solution of acryloyl chloride (0.42 mM, 5.2 mmol) was added dropwise at 0 °C to a CHCl3 (30 mL) solution of a mixture of 4-(1,2,2-triphenylvinyl)phenol (5, 910 mg, 35 mmol) and triethylamine (Et3N, 1.46 mL, 10 mmol). The resulting mixture was stirred at 25 °C for 3 h, poured into a saturated aqueous solution of NaHCO3, and then extracted with CHCl3. A combined organic extract was washed with water and brine, dried over anhydrous MgSO4, and then evaporated to dryness under a reduced pressure. The residue was subjected to column chromatography (SiO2, hexane/CHCl3 1/1 v/v) to allow the isolation of 1 as white solid (756 mg) in 72% yield: 1H NMR (400 MHz, CDCl3) δ (ppm) 7.01–7.11 (m, 15H), 6.89 (d, J = 9.0 Hz, 2H), 6.56 (dd, J = 17.3, 1.3 Hz, 1H), 6.27 (dd, J = 10.5, 17.3 Hz, 1H), 5.99 (dd, J = 10.5, 1.3 Hz, 1H). 13C NMR (100 MHz, CDCl3) δ (ppm) 164.3, 149.0, 143.7, 143.6, 143.5, 141.4, 141.3, 140.0, 132.4, 132.3, 131.4, 131.3, 128.1, 127.9, 127.8, 127.7, 126.6, 126.5, 120.7. FT-IR (KBr) ν (cm−1) 3076, 3054, 3024, 1756, 1677, 1599, 1502, 1443, 1356, 1200, 1166, 1140, 1017, 763, 748, 699, 613, 572, 498. HRMS (FAB): calcd. for C29H22O2 [M]+ m/z = 402.1620; found: m/z = 402.1617.
Typically, a dimethylformamide (DMF) solution (1.53 mL) of a mixture of monomer 1 (21.3 mg, 53 μmol), t-butyl acrylate (2, 146 μL, 1.0 mmol) and AIBN (1.7 mg, 11 μmol) was degassed by freeze-pump-thaw cycles (three times) and purged with argon. The mixture was stirred at 60 °C for 12 h, allowed to cool to 25 °C, and then evaporated to dryness under a reduced pressure. The residue was freeze-dried from toluene to afford t-Bu-PAA-TPE0.05 quantitatively as white solid (167 mg): 1H NMR (400 MHz, CDCl3) δ (ppm) 6.79–7.11 (br), 2.05–2.39 (br), 1.71–1.86 (br), 1.20–1.63 (br). FT-IR (KBr) ν (cm–1) 2979, 2935, 1731, 1481, 1457, 1393, 1368, 1257, 1149, 1034, 909, 846, 751, 701, 471, 430. Using a procedure similar to that for t-Bu-PAA-TPE0.05, t-Bu-PAA-TPE0.01–0.04 were obtained quantitatively from monomer 1, t-butyl acrylate (2) and AIBN with the corresponding monomer feed ratios. The values of Mn and PDI of t-Bu-PAA-TPEx, evaluated by GPC analysis, are summarized in Table 1.
Typically, a trifluoroacetic acid (58 μL) was added to t-Bu-PAA-TPE0.05 (10.0 mg, 78 μmol). The mixture was stirred at 25 °C for 12 h and evaporated to dryness under a reduced pressure. The residual volatile compounds were azeotropically removed with methanol (100 mL, five times) to afford PAA-TPE0.05 quantitatively as white solid (9.8 mg): 1H NMR (400 MHz, CD3OD) δ (ppm) 6.79–7.21 (br), 2.28–2.65 (br), 1.40–2.22 (br). FT-IR (KBr) ν (cm−1) 2961, 2361, 1716, 1503, 1454, 1417, 1249, 1168, 802, 701, 614, 503, 414. Using a procedure similar to that for PAA-TPE0.05, PAA-TPE0.01–0.04 were obtained quantitatively from trifluoroacetic acid and the corresponding precursors (t-Bu-PAA-TPE0.01–0.04). The composition ratios of PAA-TPE0.01–0.04, evaluated by 1H NMR spectroscopy, are summarized in Table 1.
Typically, a DMF (0.71 mL) solution of a mixture of monomer 1 (21.3 mg, 53 μmol), acrylic acid (3, 67 μL, 980 μmol), tetraethylene glycol diacrylate (4, 8.6 μL, 32 μmol) and AIBN (1.7 mg, 11 μmol) was degassed by freeze-pump-thaw cycles (three times) and purged with argon. The mixture was allowed to stand at 60 °C for 12 h and then cool to 25 °C. The resultant gelatinous material was subjected to Soxhlet extraction with a mixture of methanol/acetone (1/1 v/v) for 24 h, dried at 80 °C under a reduced pressure for 48 h, affording g-PAA-TPE0.05 as white solid (46 mg) in 48% yield. Using a procedure similar to that for g-PAA-TPE0.05, g-PAA-TPE0.01–0.04 were obtained in ~50% yield from monomer 1, acrylic acid (3), tetraethylene glycol diacrylate (4) and AIBN with the corresponding monomer feed ratios. The feed ratios for the preparation of g-PAA-TPEx are summarized in Table 1. Using procedures similar to that for g-PAA-TPEx, other crosslinked polymers (Supplementary Fig. S10) were obtained in ~50% yield from monomer 1, acrylic acid (3), corresponding crosslinker (6–8) and AIBN with the corresponding monomer feed ratios.
Evaluation of the apparent dissociation constant (K d)
Ca2+ titration curves were obtained by measuring the fluorescence intensities (for PAA-TPEx) or quantum yields (for g-PAA-TPEx) under various Ca2+ concentrations. Because the number of effective Ca2+-binding sites in PAA-TPEx and g-PAA-TPEx cannot be determined, a general stoichiometric analysis for determining the dissociation constant (Kd) is not applicable to these systems. Instead, we used the apparent Kd, which was obtained by fitting the Ca2+ titration curves with the following Hill’s equation (1) using the least square method in R software (http://www.R-project.org/).
F: Fluorescence intensity (for PAA-TPEx) or quantum yield (for g-PAA-TPEx)
Fmax: Maximum fluorescence intensity (for PAA-TPEx) or quantum yield (for g-PAA-TPEx)
Fmin: Minimum fluorescence intensity (for PAA-TPEx) or quantum yield (for g-PAA-TPEx)
Kd: Apparent dissociation constant
n: Apparent Hill coefficient
Evaluation of the swelling ratio of g-PAA-TPE x
For swelling the gel, a sliced sample was immersed in a HEPES buffer solution (70 mM, pH = 7.4) at 25 °C for 30 minutes. Swelling ratios were evaluated from the following equation (2):
Wdry: The weight of dried g-PAA-TPEx
Wswollen: The weight of swollen g-PAA-TPEx
All experimental protocols were approved by the Animal Care Committee of Nara Medical University according to the NIH (USA) guidelines and the Guidelines for Proper Conduct of Animal Experiments published by the Science Council of Japan. Experimental details are described in Supplementary Information.
How to cite this article: Ishiwari, F. et al. Bioinspired design of a polymer gel sensor for the realization of extracellular Ca2+ imaging. Sci. Rep. 6, 24275; doi: 10.1038/srep24275 (2016).
This work was supported by the Japan Science and Technology Agency (JST) Exploratory Research for Advanced Technology (ERATO) Someya Bio-Harmonized Electronics and KAKENHI (Grant-in-Aid for Research Activity Start-up No. 24850008 to F.I.). We thank Masaki Sekino, Yusuke Inoue and Dongming Kim (The University of Tokyo) for providing the fluidic device and microslicer. We thank the Material Analysis Suzukake-dai Center, Technical Department, Tokyo Institute of Technology, for high-resolution fast atom bombardment mass spectrometry and dynamic light scattering measurements.
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