Open Access Article
Anastasiia
Hubina
*a,
Yevheniia
Lobko
b,
Ivan
Khalakhan
b and
Yuliya
Khrunyk
c
aDepartment of Polymers, University of Chemistry and Technology Prague, Technická 5, Prague166 28, Czech Republic. E-mail: hubinaa@vscht.cz
bDepartment of Surface and Plasma Science, Faculty of Mathematics and Physics, Charles University, V Holešovičkách 2, Prague 180 00, Czech Republic
cInstitute of Biochemistry, Leipzig University, Brüderstraße 34, Leipzig, 04103, Germany
First published on 24th September 2025
Poly(1,2,3-triazole)-based polymers remain underexplored as a versatile platform for biomedical soft materials. Here, we report the modular synthesis of amphiphilic poly(1,2,3-triazole)-co-polytriazolium copolymers (qH-PETH) via copper(I)-catalyzed azide–alkyne cycloaddition (CuAAC) polyaddition and post-polymerization quaternization with a degree of quaternization equal to (0.85). These polymers exhibit unusual visible colouration in the absence of chromophores—appearing almost colourless in N-methyl-2-pyrrolidone (NMP), orange in DMSO, and pale orange in water—accompanied by a pronounced red shift in non-polar solvents such as dichloromethane (DCM) or chloroform. This optical behaviour is attributed to solvent-dependent supramolecular aggregation. Dynamic light scattering (DLS) measurements reveal hydrodynamic diameters of <20 nm in water and approximately 500 nm in chloroform for quaternized polymers (qH-PETH), indicating strong aggregation in low-polarity environments. UV-vis spectroscopy and atomic force microscopy (AFM) further support aggregation-induced optical effects modulated by solvent polarity and hydrogen-bonding capacity. Both neutral and quaternized polymers display excellent cytocompatibility toward human cell lines (HeLa, HEK293, THP-1) at concentrations up to 100 μg mL−1, with no detectable immunogenic activation. These findings position poly(1,2,3-triazole)-co-polytriazolium copolymers as a promising, tunable class of biocompatible soft materials for biointerface engineering and responsive biomedical applications.
1,2,3-Triazole-based polymers are readily accessible via copper(I)-catalyzed azide–alkyne cycloaddition (CuAAC) click chemistry and offer an intriguing yet underutilized opportunity.7,8 The triazole ring combines aromaticity, high dipole moment, hydrogen bonding capacity, and π-stacking propensity, facilitating supramolecular interactions and biological recognition. In small-molecule drug discovery, triazole scaffolds exhibit diverse pharmacological activities, including antifungal, anticancer, antibacterial, anti-inflammatory, and antiviral properties.3,8–11 At the same time, CuAAC strategy makes it possible to obtain versatile structures, including linear, hyperbranched, and grafted polymers. In polymeric materials, hyperbranched polytriazoles, multiarmed star polytriazoles, and AIE-active polytriazoles have enabled bioimaging, drug encapsulation, and responsive nanostructures.8,12–14 Yet, compared to other polymer classes, poly(1,2,3-triazole)s remain largely untapped in biomedical materials design.
An even more underexplored class is represented by poly(1,2,3-triazolium)s, ionic derivatives obtained by N-alkylation of polytriazoles.7 These (poly(ionic liquid)s) (PILs) possess tunable solubility, thermal stability, and ionic conductivity, having found their initial applications in electrochemical devices, membranes, and ion conductors. The studies of Drockenmuller et al., reported the substitution pattern of the triazolium ring to modulate ion transport and self-assembly behaviour.15–20 However, most publications on these polymers focus mainly on their potential as anion-exchange materials and materials for electrochemical and electrochromic applications.18,21–24 Their potential as biocompatible, responsive soft matter is largely unexplored. There are almost no reports on poly(1,2,3-triazolium)s in drug or gene delivery, or biosensing, and the impact of polymer architecture and ionic content on self-assembly has not been investigated. Similarly, there is a lack of systematic evaluations of cytocompatibility, despite growing evidence that low-molecular-weight triazolium compounds exhibit substituent-dependent biological responses.25,26
In this work, we present a new amphiphilic single-chain poly(1,2,3-triazole) polymer and its quaternized derivative poly(1,2,3-triazole)-co-polytriazolium, synthesized via CuAAC polyaddition of PEG1000-diyne and 1,6-diazidohexane segments, followed by postpolymerization N-alkylation. These polymers exhibit solvent-induced aggregation and visible solvatochromism without added dyes, arising from emergent supramolecular ordering. Dynamic light scattering (DLS), UV-vis spectroscopy, and atomic force microscopy (AFM) confirm the formation of solvent-tunable nanostructures, accompanied by a visible colour change. Critically, both the neutral and partially quaternized polytriazoles display no detectable cytotoxicity in HeLa, HEK293, and THP-1 cell lines, even at high polymer concentrations (up to 100 μg mL−1), and show no apparent immunogenic response. These results demonstrate that simple, scalable triazole chemistry followed by straightforward postpolymerization modification can yield biocompatible, optically responsive polymers with supramolecular activity. This approach could be used to design new materials for sensing, imaging, and active interfaces in soft matter and biomedicine.
Cell cultures. Human embryonic kidney (HEK) 293 cells were cultured in Dulbecco's modified Eagle's medium (DMEM)/Ham's F12 (1
:
1) (Lonza, Basel, Switzerland) supplemented with 15% fetal bovine serum (FBS) (Biochrom GmbH, Berlin, Germany). Human cervix carcinoma (HeLa) cells were cultured in RPMI 1640 (Lonza) supplemented with 10% FBS. A suspension cell line THP-1 was cultured in RPMI 1640 (10% FBS and 10 mM glutamine, Lonza). All cells were maintained in T75 cell culture flasks at 37 °C, 95% humidity, and 5% CO2 (standard conditions). These cell lines were used for no more than 15 passages. Medium was changed every 4–5 days.
000/well), seeded into 96-well cell culture plates (i.e. THP-1 in Greiner (Kremsmünster, Austria) with non-binding surfaces, HeLa and HEK293 in TPP (Trasadingen, Switzerland)), were cultured in respective media containing tested compounds in various concentrations: 0, 0.78, 1.56, 3.125, 6.25, 12.5, 25, 50, and 100 μg mL−1. Following 24 h of incubation, cell culture medium was aspirated, cells were rinsed with PBS, and further incubated with 100 μL of a sterile resazurin solution (0.0025% in PBS) (Sigma-Aldrich, St. Louis, MO, USA) at 37 °C. In parallel, aiming to evaluate the viability of a total amount of THP-1 cells (i.e., adhered and non-adhered), resazurin solution (100 μL) was added directly to the cell suspension. THP-1 cells induced by phorbol 12-myristate 13-acetate (PMA, Thermo Fischer Scientific (Ward Hill, MA, USA), 200 nM) were used as a positive control. The resulting fluorescence (excitation λ: 550 nm, emission λ: 595 nm) was measured using a Tecan Spark multimode microplate reader (Tecan Group, Männedorf, Switzerland) after incubation for 30 min, 60 min, 90 min, and 120 min. Blank values obtained for the respective conditions without cells were subtracted from the obtained fluorescence data.
C-CH2-), 3.74–3.60 (m, 88H, -O-CH2-CH2-), 2.47 (t, 2H, HC
C-CH2-), (Fig. S1A).
C-CH2-), 3.59–3.39 (m, 88H, -O-CH2-CH2-), 1.77 (s, 4H triazole-CH2-CH2-CH2-), 1.27 (s 4H triazole-CH2-CH2-CH2-), (Fig. S1C).
The synthesized PETH polymer, as characterized by SEC, exhibited an apparent number-average molecular weight (Mn) of approximately 9900 g mol−1 and a weight-average molecular weight (Mw) of 14
000 g mol−1, indicating a moderate molecular weight distribution (Đ =1.42) consistent with step-growth polyaddition (SI Fig. S3).
C-CH2-), 3.68–3.4 (m, 88H, -O-CH2-CH2-), 1.9 (m, 4H triazole-CH2-CH2-CH2-, 8H, triazolium-CH2-(CH2)4-CH3), 1.2 (s 4H triazole-CH2-CH2-CH2-), 0.8 (m, 3H, triazolium-CH2-(CH2)4-CH3) (Fig. S1D).
The degree of quaternization was calculated from 1H NMR spectrum of qH-PETH (SI Fig. S1D) as follows: DQ = (Ic′)/(Ic + Ic′), where c′ is proton in triazolium ring and c is a proton in triazole ring. Calculated DQ is 0.85.
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| Scheme 1 Synthesis of α,ω-PEG1000-dyine, 1,6-diazidohexane, poly(ethylene glycole-triazole-hexyl) (PETH), partially hexyl-quaternized poly(ethylene glycole-triazole-hexyl) (qH-PETH). | ||
In solvents such as DMSO, acetone, and acetonitrile, qH-PETH shows a rich orange hue (absorbance at ∼512 nm), indicative of self-assembly-driven chromophore-like behaviour. This behaviour is likely due to interactions between triazolium moieties and their hydrophobic tails. In contrast, in highly polar and strongly solvating media e.g. NMP and water, the solutions appear almost colourless (weak absorbance at 485 nm in NMP), suggesting good solvation of the polymer chains and the disruption of the aggregation responsible for solvatochromism. While in water H-bonding leads to formation of nanoparticles ∼10 nm size and absorption peak at (476 nm).
The neutral polymer PETH, by comparison, shows more uniform and less intense colouration across all solvents, supporting the idea that ionic character and amphiphilic structure in qH-PETH amplify its solvent-responsive behaviour. These visual trends are consistent with spectroscopic data (Fig. 1(C) and (D)) and point toward solvent-mediated morphological changes as the key mechanism behind the observed solvatochromism.
The aqueous solutions of qH-PETH are of particular interest for potential biomedical applications; therefore, we investigated their colloidal stability across a relevant concentration range. Dynamic light scattering and UV-vis spectroscopy revealed that between 0.25 and 1.0 mg mL−1, both the particle size and absorption maximum remained unchanged, indicating robust aggregation behaviour (Fig S6). Furthermore, time-dependent studies demonstrated excellent stability, particle size did not demonstrate significant change after 48 h, with the results corroborated by a consistent zeta potential modulus of approximately 40 mV (Fig. S7).
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| Fig. 2 Contour plots of polymer particles size correlation with Kamlet–Taft parameters of the solvents of PETH (A) and (B) and qH-PETH (C) and (D). | ||
The dependence of aggregate size of the neutral polymer PETH on solvent properties is illustrated in the contour plots correlating particle size (all the DLS data is available in the SI). Fig. 2 shows the Kamlet–Taft parameters α (HBD) (Fig. 2A), β (HBA) (Fig. 2B), and π* (dipolarity/polarizability). In this case, aggregate formation does not correlate simply with solvent polarity: while relatively small particles are observed in moderately polar aprotic solvents such as acetone, ACN, and THF, the largest aggregate sizes occur in highly polar and strongly hydrogen-bonding solvents such as NMP and water. This suggests that hydrogen bonding and polymer–polymer association dominate in these environments, possibly due to partial desolvation of hydrophobic domains and promotion of interchain interactions through hydrogen bonding networks. In contrast, in low polarity, weakly hydrogen-bonding solvents (DCM, chloroform), moderate to large aggregates also form through hydrophobic-driven self-assembly. Overall, the behaviour of the neutral polymer reflects a complex balance between polarity and hydrogen-bonding effects, rather than a simple polarity-driven solubility trend.
For the charged polymer qH-PETH, the aggregation behaviour exhibits a more systematic dependence on solvent polarity. As seen in the contour plots, the particle size increases progressively along the solvent polarity sequence: dioxane < THF < acetone < ACN < NMP < DMSO, demonstrating that increased polarity promotes interchain interactions and aggregation in these aprotic solvents. This trend likely reflects the decreased ability of aprotic polar solvents to fully shield the ionic groups and hydrophobic segments simultaneously, favouring associative interactions. However, in water, the behaviour is strikingly different: extremely small particles are formed, suggesting the presence of highly solvated, potentially single-chain particles stabilized by strong hydrogen bonding with the aqueous environment. This distinct behaviour highlights the critical role of hydrogen-bond donor capacity (α) in promoting molecular dispersion of the charged polymer in water, being in sharp contrast to its aggregation tendency in polar aprotic solvents.
In conclusion, while the neutral polymer PETH exhibits a complex aggregation pattern influenced by both hydrophobic interactions and hydrogen bonding, the charged polymer shows a clear polarity-dependent aggregation trend in aprotic solvents, with water uniquely favouring molecular dispersion. This illustrates how charge and solvation effects fundamentally alter the self-assembly landscape of two polymer systems.
To clarify the influence of both polarizability and H-bonding, we prepared two series of qH-PETH sample in water mixed with other solvent in various ratios, first with DMSO considering that two solvents have close polarity but extremely different proton donating ability (HBD) (Fig. 3). The dual-axis plot illustrating particle size and absorption maximum (λmax) in DMSO/water mixtures reveal a strong correlation between aggregation and solvatochromic behaviour, governed by the solvent environment's Kamlet–Taft parameters. As the DMSO content increases (i.e., α decreases and β increases), the particle size rises sharply, indicating enhanced aggregation. This trend reflects the poor hydrogen bond donor (HBD) capacity of DMSO (α = 0.00), which fails to stabilize the charged and hydrophilic segments of the polymer, thus promoting interpolymer interactions and self-assembly. Concurrently, the absorption maximum undergoes a redshift, consistent with the formation of larger, more ordered aggregates which suggest that solvatochromism is aggregation-induced. In contrast, high water content (α = 1.17, β = 0.47) leads to minimal aggregation and a blue-shifted λmax, pointing to the presence of molecularly dispersed chains in a strongly hydrogen-bonding medium. These findings demonstrate that solvent polarity and hydrogen-bonding parameters, especially α, critically govern both the size and optical response of the polymer assemblies.
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| Fig. 3 Dependence of particle size (black) and UV-vis absorption maximum (red) of the qH-PETH in DMSO/water mixtures (0.25 mg mL−1). | ||
These observations were further supported by AFM images of the samples prepared from the same solutions (Fig. 4). In water and in mixtures with higher water content, qH-PETH forms nanoparticles, probably single-chain. As the water content decreases as well as α (αH2O = 1.17, αDMSO = 0), the biggest aggregates, probably micelle-like, are formed mainly due to hydrophilic–hydrophobic interactions.
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Fig. 4 AFM images of qH-PETH solutions (0.25 mg mL−1) in DMSO/water mixtures: A – 0/100; B – 25/75; C – 50 : 50; D – 75/25. | ||
These results suggest that by tuning solvent polarity and hydrogen-bond donor capacity, it is possible to control the transition between discrete, molecularly dispersed chains and self-assembled aggregates of the charged polymer. Such control over aggregation behaviour could be further explored for designing systems where triggered disassembly or size modulation is desirable, for example, in intracellular delivery or responsive release formulations.
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| Fig. 5 qH-PETH solutions in water and dioxane: A – UV-vis spectra, B – particle size distribution according to DLS. | ||
According to AFM images of the water/dioxane mixtures (Fig. 6), the self-assembly follows a distinct path. The polymer is well-dissolved in pure dioxane, forming a smooth polymer film, no aggregation is also observed at 75% dioxane content. As water content increases, particle-like features begin to appear, with the most pronounced and uniformly distributed spherical assemblies emerging at 100% water.
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Fig. 6 AFM images of qH-PETH solutions (0.185 mg mL−1) in water/dioxane mixtures: A – 100/0; B – 75/25; C – 50 : 50; D – 25/75; E– 0/100. | ||
This difference in aggregation behaviour, compared to DMSO/water systems, reflects the solvent's ability to mediate intermolecular interactions. Dioxane, being less polar and less hydrogen-bonding than DMSO, facilitates sharper transitions in morphology upon water addition. These findings further demonstrate the polymer's sensitive and tunable self-assembly profile driven by solvent polarity and hydrogen-bonding capacity, supporting the potential of qH-PETH as a responsive nanomaterial platform.
In both DMSO/water and dioxane/water solvent systems, DLS measurements reveal a progressive decrease in particle size as the water content increases, consistent with a transition from a molecularly dissolved state to well-defined nanostructures.
Although the polymer lacks conventional chromophores, UV-vis spectra still show notable changes in the visible region with solvent composition. These subtle spectral shifts and intensity changes are most likely due to aggregation-induced modulation of the electronic environment, for instance, alterations in local dielectric constant, dipole orientation, or short-range packing between quaternized triazolium groups and surrounding PEG segments. The intensity increase in more aqueous conditions aligns with the formation of ordered aggregates, as observed by AFM and supported by DLS.
After 24 hours of cultivation, the mitochondrial activities of cells incubated with tested compounds were analyzed by resazurin conversion to resorufin (Fig. 7 and 8). To test an immunogenic and/or allergenic potential of PETH and qH-PETH, THP-1 suspension cells (the human leukaemia monocytic cell line) were employed as a model of monocyte-to-macrophage differentiation.28 After incubation with various concentrations of PETH and of qH-PETH, THP-1 cell suspension was aspirated to detect the viability of only adhered cells (Fig. 7A and 8A). THP-1, exposed to PMA, which induces a rapid cell adhesion and their differentiation into cells with a macrophage-like phenotype,28 were used as a positive control. In contrast to a positive control showing dramatically elevated levels of RFU (Fig. 7A and 8A), for all PETH and qH-PETH concentrations tested, no increase in adhered THP-1 cells was detected, and the observed RFU levels were comparable to those for untreated cells. Furthermore, the range of concentrations of both compounds used for this assay did not induce cytotoxicity in THP-1, as was shown by a resazurin reduction of both adhered and non-adhered cells (Fig. 7B and 8B). The results indicate that PETH and qH-PETH (at the tested concentrations) might not induce a monocyte recruitment and their subsequent activation into macrophages.
Potential cytotoxic effects of PETH and qH-PETH were further tested employing human cervical cancer cell line HeLa (Fig. 7C and 8C) and a human embryonic kidney cell line HEK293 (Fig. 7D and 8D). To data obtained for HeLa, no toxic impact on cell viability was observed for PETH up to its highest concentration used (100 μg mL−1, Fig. 7C). The same concentration of qH-PETH resulted in a decreased RFU level of HeLa, but not to a significant level. All the other concentrations of qH-PETH tested, however, did not affect HeLa cell viability (Fig. 8C). Both compounds, PETH and qH-PETH, tended to slightly reduce HEK293 viability in a concentration-dependent manner (Fig. 7D and 8D), but not to a significant level.
Thus, the systematic analysis of solvents' effects using Kamlet–Taft parameters, together with direct visualization by AFM and a demonstration of excellent cytocompatibility, positions this class of polymers as highly promising platform for the development of responsive biointerfaces and sensing materials. These findings essentially expand the functional scope of polytriazole-based polymers beyond their current applications, establishing a new modular design paradigm for stimuli-adaptive soft materials.
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