Christina M.
Geiselhart
ab,
Hatice
Mutlu
*ab,
Pavleta
Tzvetkova
c and
Christopher
Barner-Kowollik
*bde
aSoft Matter Synthesis Laboratory, Institut für Biologische Grenzflächen 3, Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76344 Eggenstein-Leopoldshafen, Germany. E-mail: hatice.mutlu@kit.edu
bMacromolecular Architectures, Institut für Technische Chemie und Polymerchemie, Karlsruhe Institute of Technology (KIT), Engesserstraße 18, 76128 Karlsruhe, Germany
cInstitute for Organic Chemistry and Institute for Biological Interfaces 4 – Magnetic Resonance, Karlsruhe Institute of Technology (KIT), Hermann-von-Helmholtz-Platz 1, 76344 Eggenstein-Leopoldshafen, Germany
dCentre for Materials Science, Queensland University of Technology (QUT), 2 George Street, Brisbane, QLD 4000, Australia. E-mail: christopher.barnerkowollik@qut.edu.au
eSchool of Chemistry and Physics, Queensland University of Technology (QUT), 2 George Street, Brisbane, QLD 4000, Australia
First published on 19th May 2020
We introduce the synthesis of a self-reporting system with chemiluminescent output, which is regulated via dynamic supramolecular complex formation. By free radical polymerization and subsequent post-polymerization modification, a copolymer decorated with luminol and superbase (i.e. 1,5,7-triaza-bicyclo-[4.4.0]dec-5-ene (TBD)) moieties was synthesized, which in turn forms supramolecular host–guest-complexation with randomly methylated β-cyclodextrin (Me-β-CD). Upon hydrogen peroxide addition, the host–guest-interactions with the self-assembly are broken, and the luminol is oxidized to 3-aminophthalic acid (3-APA). Critically, no additional base, buffer or catalyst is required to generate the striking blue light emission of the polymeric system that is detectable by the naked eye. Thus, a fast and easy detection of reactive oxygen species (ROS), such as hydrogen peroxide, under mild conditions is established. The self-reporting system and its chemiluminescent properties are characterized by 1D and 2D NMR spectroscopy (particularly NOESY), dynamic light scattering (DLS), UV/Vis spectroscopy and chemiluminescence (CL) measurements.
Between the different types of self-reporting phenomena, chemiluminescence (CL) has been recognized as a functional tool due to its high sensitivity and wide dynamic range without the requirement of sophisticated equipment.9–11 Besides common luminophores such as dioxetanes,12 peroxyoxalates4 or acridinium compounds,13 luminol has gained significant attention since its discovery by Albrecht in 1928,14,15 due to its low cost, beneficial properties and wide-ranging applications. Unfortunately, the quantum yield of luminol is rather low (≈0.01 in aqueous media and ≈0.09 in DMSO),16 therefore substantial efforts have been devoted to develop new luminol systems with higher CL emission. Indeed, the latter is achievable by substituting the aromatic ring of luminol with adequate molecules or by utilizing distinctive catalysts, such as organic frameworks17,18 or nanoparticles.19,20
Recently, we successfully implemented the organic superbase 1,5,7-triaza-bicyclo-[4.4.0]dec-5-ene (TBD) into the CL reaction of luminol.21 Without the requirement for additional additives (such as catalysts or enhancers), the CL of a luminol–TBD-mixture in organic media (DMSO) was readily triggered in the presence of hydrogen peroxide (H2O2). Indeed, the resulting CL of the system can be observed by the naked eye. Therefore, we submit that by fusing the properties of luminol and TBD within one polymeric backbone, the synthesis of polymeric self-reporting CL systems triggered by oxidants such as H2O2, would be feasible. Especially in the field of biomedicine and diagnostics, the fast and ready detection of H2O2 is critical, since its increased level is a sign for oxidative stress and diseased cells.22,23
In order to construct the self-reporting CL system with relevance to the aforementioned applications, we expanded our superbase driven luminol concept further by constructing supramolecular assemblies based on a luminol–TBD–polymer with tailor-made supramolecular host-molecules. Host–guest binding is analogous to the way many biomolecule–substrate interactions occur,24,25 thus supramolecular assemblies based on diverse host–guest interactions are of key interest and find widespread applications in biomedicine, drug delivery, catalysis, nanotechnology molecular recognition or sensor technology.26–30 Wild cyclodextrins (CD) as well as their chemically modified variants have proven to be able to encapsulate biomolecules (such as amino acids) to form supramolecular self-assemblies.31–33 Especially the guanidine-functional group in the essential amino acid L-arginine enables selective host–guest inclusion complexes with β-CD.34,35 We thus consider a possible inclusion of the guanidine-functionality in TBD with β-CD. In addition, CDs are efficient boosters for the CL of luminol.36–38
Synthetically, the luminol–superbase–polymers were obtained via a post-polymerization modification (PPM) approach. In fact, PPMs have been proven to be a useful tool to synthesise highly functionalized polymers, especially since conventional polymerization processes do not allow the direct polymerization of monomers decorated with multiple functional groups.39–41 In addition to synthetic polymers, commercially available polymers (e.g. polybutadiene42) can be decorated with a broad variety of functionalities to obtain innovative macromolecules with tailor-made properties. Among the different reactions enabling PPMs (copper-catalyzed azide–alkyne cycloaddition (CuAAC),43 thiol–ene addition,44 Michael addition,45 or electrophilic cascade reactions42), active esters, such as pentafluorophenyl (PFP) esters,46–48 are considerably attractive functional units to deliver well-defined multi-functionalized polymers. Especially the possibility to modify active PFP ester groups within a copolymer backbone in a precise and orthogonal manner is highly beneficial.49
Herein, via free radical polymerization (FRP) of two different active PFP ester monomers in the presence of methyl methacrylate (MMA), and subsequent orthogonal PPM, we are able to synthesize the luminol–superbase copolymers P1 and P2, as illustrated in Scheme 1. To evidence the concept of a supramolecular self-reporting CL-system with tuneable supramolecular complexation properties and to gain insights into the structural influence of the employed superbase, an acyclic (G3 in Scheme 1A) and a cyclic (namely TBD, Scheme 1B) guanidine derivative were evaluated. In-depth characterization of the supramolecular self-reporting CL-systems were performed using NMR (1D and 2D) spectroscopy, DLS and UV/Vis spectroscopy. Furthermore, CL measurements were utilized to reveal the efficiency as self-reporting systems.
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Scheme 1 Synthetic route to the luminol–superbase polymers P1 (A) and P2 (B) via free radical polymerization and subsequent post-polymerization modification with luminol and the respective superbase. |
On the one hand, the synthesis of the luminol–guanidine–copolymer P1 (displayed in Scheme 1A) was confirmed via 1D NMR analysis of the purified copolymer. Critically, all relevant resonances assignable to the respective protons of P1 were detected in the 1H NMR spectrum (Fig. S2 in the ESI†). In addition, the 19F NMR spectrum (Fig. S2 in the ESI†) confirmed that all active PFP ester moieties were substituted by the luminol and guanidine-functionalities. The resonance at −75 ppm is associated with the TFA utilized during the monomer synthesis. On the other hand, P1 is not soluble in typical organic solvents employed for SEC (such as THF or DMAc), thus the apparent number average molecular weight and the dispersity values of P1 could not be determined via SEC.
In order to obtain the luminol–TBD–copolymer P2 with efficient CL to be detected by the naked eye, the monomer choice employed for the PPM approach of P1 was slightly altered. Thus, a copolymer of MMA, PFPA and 4-vinyl benzylchloride (VBC) was synthesized via FRP (refer to Scheme 1B). Subsequently, P2 was obtained by the orthogonal PPM of the PFPA moiety with luminol and substitution of VBC with TBD, respectively. The successful synthesis of P2 was confirmed by 1D NMR spectroscopy, as shown in Fig. S3 in the ESI.† Importantly, the resonances of the NH-protons of luminol (i, h′) and TBD (w), as well as the resonances of h, m, n, and o of P1 in Fig. S2,† were intense compared to resonance of methylene spacer (i.e., t), which resulted from the electrostatic interactions in the delocalized charge of each (de-)protonated species, and furthermore with the increased pH value of the environment that is basic due to excess of guanidine units. Similar to P1, the measurement of the apparent number average molecular weight of P2 remained elusive via conventional SEC eluents.
Whereas the definition of size and thus molecular weight, measured by dynamic light scattering (DLS) differs from that of SEC, due to the inherent limitation of intensity-biased detection, we have validated the hydrodynamic radii (Rh) of P1 and P2via DLS analysis. While the average radii of P1 was 4.4 nm at a copolymer concentration of 1 mg mL−1 (red trace in Fig. 1), the corresponding value for P2 (blue trace) is close to twice the size of P1, e.g. 10.6 nm. These results are in accordance with the SEC results of the active ester copolymers AEC1 and AEC2 (refer to Scheme 1), which in contrast to P1 and P2 were soluble in typical SEC eluents (i.e. THF). As shown in Fig. S4 in the ESI,† the apparent average molecular weight of AEC2 (Mn = 14600 Da) was twice the size of AEC1 (Mn = 7720 Da). Despite the different average molecular weights, the number of repeating units and thus the number of active species incorporated into each polymer remains constant, allowing for a comparison of the resulting chemiluminescent properties.
For the complexation reaction, the respective luminol–superbase–copolymer was dissolved in DMSO, succeeded by the addition of Me-β-CD to obtain the supramolecular assemblies of C1 and C2 as depicted in Scheme 2. The key indication for a successful host–guest-complexation comes from 1H NMR spectra (refer to Fig. 2A and B). For C1 (Fig. 2A), a broadening of the resonances e and m at 8.5 ppm and of the resonances i and o at 7.8 ppm suggest interactions of the guanidine- and luminol-functionality with the Me-β-CD. Similarly, the resonances of the luminol- (i, h′) and TBD-protons (u, v, w) are broadening in the presence of Me-β-CD (Fig. 2B). It should be noted that due to solubility issues of P1 and P2, different deuterated solvents were used for the NMR analysis of C1 and C2. Whereas the spectra of P1/C1 were recorded in DMF-d7, the spectra of P2/C2 were analysed in DMSO-d6, resulting in (de-)protonated luminol- and guanidine moieties in P1/C1 and P2/C2.
Further insight into the complexation process is obtained from NOESY analysis. The recorded spectra of C1 and C2 are displayed in Fig. 2C and D. As expected, there are cross-resonances (i.e. NOEs) at 8.5 ppm (green and orange circles in Fig. 2C and D), assigned to the anticipated dominant dipolar interaction between the Me-β-CD annular protons and the guanidine derivative (either acyclic or cyclic one). Additional cross-resonances at 7.5 ppm (blue circles in Fig. 2C and D) are detectable, which arise from the interactions of the Me-β-CD with the luminol moiety both for C1 and C2. The cross-resonance at 4.5 ppm can be assigned to a complexation of the MMA moieties or further superbase functionalities by the Me-β-CD (black circles in Fig. 2C and D). Although only a supramolecular assembly of the superbase-functionality with the host-molecule was expected, the complexation of the superbase-, luminol- and MMA-moieties by the Me-β-CD in the polymer backbone clearly evidences the competence of the luminol–superbase–polymers to form supramolecular assemblies.
Supplementary to NMR analysis, DLS was used as a basis for assessing the inclusion process. Indeed, the comparison of the DLS traces of the individual components (P1, P2 and Me-β-CD) with C1 and C2 (refer to Fig. 1) support the formation of host–guest-complexes. As evident from the single DLS measurements depicted in Fig. S6 in the ESI,† only one distribution is obtained for C1 and C2, respectively. If the encapsulation did not take place with the aid of Me-β-CD, the DLS data should reveal two distinguishable distributions, one associated with the non-encapsulated polymer derivative, the other one exclusively for Me-β-CD. According to the literature, the diameter of the supramolecular complexes should lie between the diameters of the individual components prior to the complex formation.55 As illustrated in Fig. 1, the diameters of C1 and C2 lie in between the diameters of Me-β-CD and the corresponding luminol–superbase–polymer. The results also reveal that the supramolecular interactions between TBD and Me-β-CD have a higher influence for the hydrodynamic diameter of the host–guest-complexes than the interactions between guanidine and Me-β-CD, respectively. In case of the luminol–TBD–system, the hydrodynamic diameter of C2 is 51% lower than the one of P2, while the difference in the luminol–guanidine system is only 21%.
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Fig. 3 UV/Vis spectra of P1/C1 and P2/C2 (c(P/C) = 3.25 × 10−6 mmol mL−1) before and after addition of H2O2 (1 mol L−1). All spectra were recorded in DMSO at ambient temperature. |
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Fig. 4 CL emission of C1, C2 and P2 (c = 3.25 × 10−4 mmol mL−1) in DMSO at ambient temperature, triggered by 0.1 mL H2O2 (1 mol L−1). |
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Fig. 5 NOESY spectra of A: C1 + H2O2 in DMF-d7, and B: C2 + H2O2 in DMSO-d6. All spectra were recorded at 300 K. |
Similarly, the CL properties of C2 were investigated. The DLS results clearly exhibit an alternation of the host–guest interactions after the addition of H2O2 (refer to Fig. 1 and Fig. S6 in the ESI†). Upon addition of 0.1 mL H2O2 (1 mol L−1), the hydrodynamic size of C2* is 47% larger than the one of C2 and close to the size of P2 (7% difference). Presumably, in contrast to the luminol–guanidine–polymer, the new complex C2* is formed as depicted in Scheme 2 with host–guest interactions between the oxidized luminol and Me-β-CD, in accordance with the results of the NOESY spectrum of C2* displayed in Fig. 5B. As in the spectrum of C1*, there is a cross-resonance at 10.5 ppm (grey box), which can be assigned to interactions between H2O2 and Me-β-CD or the polymer backbone, and there is no detectable cross-resonance between Me-β-CD and TBD, respectively. The cross-resonance in the aromatic region (blue box) is indicating interactions between the oxidized luminol and Me-β-CD, thus supporting the DLS results. The CL emission of C2 is higher than the one for C1 (∼760 times), as pictured in Fig. 4 (blue line). Consequently, the light output is visible by the naked eye, enabling a fast and easy detection of the oxidized luminol in the presence of ROS (i.e. H2O2). Additionally, the CL emission of P2 without Me-β-CD has been recorded (green line in Fig. 4) in order to evaluate the effect of Me-β-CD on the CL reaction of luminol. As expected, a (∼140 times) higher CL emission is obtained for C2 compared to P2, underpinning the enhancing effect of Me-β-CD.
A plausible explanation for the immense difference in the CL emission between C1 and C2 lies in the structural difference of the superbase tethered to the polymer backbone. As reported in the literature,21 the type of the superbase plays a critical role in the CL reaction of luminol, not only as catalyst but also as co-reactant. While the non-cyclic guanidine-derivative in P1/C1 is transformed to the urea functionality in the presence of an oxidant (e.g. H2O2), TBD in P2/C2 remains intact due to its bulkiness. Therefore, the generated urea derivative acts no longer as a base or catalyst, thus hindering the CL reaction of luminol.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0py00332h |
This journal is © The Royal Society of Chemistry 2020 |