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Design and evaluation of a thiazoline-appended imidazole based fluorescent turn on chemosensor for Hg2+ ion detection: spectroscopic characterization and solid state film applications

Bharathkumar Thangaraja, Suresh Ranganathanbc, Ravichandran Cingarama, Lakshmipriya Kannana, Sathiyanarayanan Kulathu Iyerd and Karthikeyan Natesan Sundaramurthy*a
aDepartment of Chemistry, Easwari Engineering College, Chennai, India. E-mail: karthikeyan.ns12@gmail.com
bDepartment of Chemistry, Karpagam Academy of Higher Education, Coimbatore, India
cCentre for Material Chemistry, Karpagam Academy of Higher Education, Coimbatore, India
dChemistry Division, School of Advanced Sciences, Vellore Institute of Technology, Chennai, India

Received 9th April 2026 , Accepted 26th May 2026

First published on 1st June 2026


Abstract

Mercury contamination presents a significant environmental and biological hazard, necessitating the development of reliable and sensitive fluorescent probes for the detection and removal of mercury ions. In this study, a novel fluorogenic chemosensor (BTA) incorporating a sulfur- and nitrogen-donor analogue of 4-(bis(2-((4,5-dihydrothiazol-2-yl)thio)ethyl)amino)benzaldehyde, has been synthesized for the selective detection of Hg2+ ions. BTA exhibits excellent chemo-selectivity and high sensitivity towards Hg2+ ions in a binary mixture of acetonitrile–water medium (CH3CN[thin space (1/6-em)]:[thin space (1/6-em)]H2O) (6[thin space (1/6-em)]:[thin space (1/6-em)]4, v/v), showing a distinct red shift (∼15 nm) in absorption spectrum and a pronounced fluorescence “turn-on” response. The detection limit was determined to be 114.7 nM, confirming its superior analytical performance. Detailed spectroscopic investigations, including Job's plot, proton NMR titration, HR-MS, FT-IR, and DFT calculations, confirm a 1[thin space (1/6-em)]:[thin space (1/6-em)]1 binding stoichiometry between BTA and Hg2+. The probe displays a prompt emission response, excellent reversibility, and strong anti-interference capability. Moreover, a Boolean logic gate (AND) was developed using the emission response of BTA to achieve selective detection of Hg2+ ions. Furthermore, a BTA infused PVA solid-state fluorescent film (BTA/PVA) was developed, enabling efficient recognition of deadly Hg2+ under practical conditions.


Introduction

Mercury poisoning remains a severe environmental and health problem, owing to its persistence, extreme toxicity, and bioaccumulative tendency, even at minimum concentration. The divalent mercury ions (Hg2+) are predominantly hazardous because it quickly binds with sulfur and nitrogen-containing biomolecules, causing protein denaturation and disruption of enzymatic and neuronal activities.1–3 Exposure to Hg2+ has been connected with vital physiological processes, resulting in severe disorders such as neurotoxicity, nephrotoxicity, hepatotoxicity, and developmental abnormalities, stressing the crucial need for effective and rapid detection methods.4–7

Various advanced analytical instrumentation techniques, including atomic absorption spectroscopy (AAS),8 anodic stripping voltammetry (ASV),9 γ-ray spectrometry,10 inductively coupled plasma mass spectrometry (ICP-MS)11 and electrophoresis12 have been used for mercury detection. Although these methods provide outstanding precision and sensitivity, their practical value is limited by expensive instrumentation, trained operators, time-consuming sample preparation, and lack of portability, rendering them unsuitable for routine or on-site detection.13,14 Therefore, the development of facile, cost-effective, and rapid sensing approaches capable of detecting Hg2+ ions with high sensitivity and selectivity under ambient conditions remains an important goal.15–17 As a result, fluorescent chemical sensors have materialized as powerful substitutes due to their high sensitivity, operational simplicity, fast response time, with potential visual detection.18 Various organic chemoprobes, including rhodamine,19 BODIPY,20 coumarin,21 phenanthridine,22 triphenylamine (TPA),23 imidazole,24 Schiff's base25 and thiazoline derivatives have been exploited for mercury sensing through diverse mechanisms such as photoinduced electron transfer (PET), aggregation-induced emission (AIE), metal-induced fluorescence enhancement or quenching and intramolecular charge transfer (ICT).26,27 However, our study focuses on imidazole-based probes, as several previously documented probes suffer from drawbacks, such as turn-off responses, solvent dependence, and exhibits poor performance.28–32 In contrast, the probe BTA displays a fluorescence “turn-on” response to Hg2+ with high sensitivity and selectivity. Moreover, its successful integration of BTA into PVA addressing key constraints of previous methods.

In this work, we report the design and synthesis of a novel sulfur- and nitrogen-rich fluorogenic probe (BTA), derived from the reaction of 4-(bis(2-((4,5-dihydrothiazol-2-yl)thio)ethyl)amino)benzaldehyde and benzil. The probe exhibits pronounced selectivity and sensitivity toward Hg2+ ions in an aqueous acetonitrile medium, accompanied by an intense fluorescence enhancement. In addition, BTA integrated poly(vinyl alcohol) (PVA) matrix yields a fluorescence ON robust solid-state film sensor capable of selective detection of Hg2+ ions, offering a promising strategy for practical, on-site mercury monitoring applications.33

Experimental section

Reagents and instruments

Unless otherwise specified, all reagents and solvents were obtained from commercial suppliers and used without further purification. Thin-layer chromatography (TLC) was performed on silica gel 60 F254 plates to monitor reaction progress. 1H NMR and 13C NMR spectra of BTA were recorded on a Bruker 400 MHz spectrometer using tetramethylsilane (TMS) as an internal reference, and chemical shifts (δ) are reported in parts per million (ppm). FT-IR spectra were recorded on a JASCO-4100. High-resolution mass spectrometry data were obtained using a WATERS XEVO G2-XS QToF mass spectrometer. UV-visible absorption spectra were recorded on a JASCO V-750 spectrophotometer, while emission spectra were obtained using a JASCO FP-8300 spectrofluorometer at ambient temperature. All metal ion stock solutions were freshly prepared for analytical measurements using deionized water.

Preparation of stock and working solutions

BTA was dissolved in an acetonitrile–water mixture (CH3CN[thin space (1/6-em)]:[thin space (1/6-em)]H2O = 6[thin space (1/6-em)]:[thin space (1/6-em)]4, v/v) to prepare a 1 mM stock solution, which was subsequently diluted to 20 µM for UV-visible and fluorescence spectroscopic studies. Solutions of various ions, including Hg2+, Ni2+, Na+, Mo6+, Li+, Mn2+, Mg2+, K+, Fe2+, Cd2+, Ca2+, Zn2+ Co2+, Ba2+, Ag+, Sr2+, W6+, Br, Cl, CN, F, HS, I, SCN, NO2, H2PO4, HSO4, and NO3 ions were prepared at 1 mM concentrations in deionized water and used as analytes. The excitation wavelength for emission measurements was set at 325 nm, and all spectral experiments were carried out at room temperature using the same solvent composition (CH3CN[thin space (1/6-em)]:[thin space (1/6-em)]H2O = 6[thin space (1/6-em)]:[thin space (1/6-em)]4, v/v).

Synthesis of chemoprobe BTA

The synthetic pathway for chemoprobe BTA is illustrated in Scheme 1. The 2 TA was obtained using a method adapted from a previously published procedure.4 Briefly, benzil (0.12 g), 2 TA (0.3 g), and ammonium acetate (0.45 g) were dissolved in 25 mL of glacial acetic acid (AcOH) and the reaction mixture was refluxed for 6 h with constant stirring. The completion of reaction was monitored by TLC method, then the mixture was cool to ambient temperature, and extracted three times with chloroform (3 × 30 mL). The organic layers were dried over anhyd. NaSO4, and concentrated under reduced pressure. The crude residue was purified by column chromatography using hexane/ethyl acetate (6[thin space (1/6-em)]:[thin space (1/6-em)]4 v/v) solvent system. The desired compound (BTA), was obtained as a yellow solid in 75% yield. The structure of BTA was confirmed by 1H NMR, 13C NMR, FT-IR, and HR-MS analyses (Fig. S3–S6). 1H NMR (400 MHz, DMSO-d6), δ (ppm): 12.35 (1H), 7.92–7.90 (2H), 7.53–7.35 (10H), 7.05–7.03 (2H) 4.26–4.22 (4H), 3.68–3.65 (4H), 3.52–3.48 (4H), 3.30–3.26 (4H); 13C NMR (100 MHz, DMSO-d6) 172.48, 163.61, 147.43, 146.83, 128.83, 127.04, 119.05, 112.13, 64.48, 50.16, 35.84, 29.47, 21.52. IR: 2916 cm−1, 1566 cm−1, 1496 cm−1, 1284 cm−1, 1134 cm−1, 956 cm−1, 690 cm−1, and; HR-MS for C31H31N5S4 calc. [M]+ m/z, 601.1462; experimental value [M + H]+ m/z, 602.1542.
image file: d6ra03004a-s1.tif
Scheme 1 Schematic representation for synthesis of probe BTA.

Results and discussion

Spectroscopic insights into the sensing performance of BTA

The sensing features of the newly designed chemoprobe BTA were systematically examined to evaluate its selectivity and sensitivity towards diverse metal ions. To assess its sensing property, both UV-visible and fluorescence spectroscopy were performed in the presence of series metal cations and anions, including Hg2+, Ni2+, Na+, Mo6+, Li+, Mn2+, Mg2+, K+, Fe2+, Cd2+, Ca2+, Zn2+ Co2+, Ba2+, Ag+, Sr2+, W6+, Br, Cl, CN, F, HS, I, SCN, NO2, H2PO4, HSO4, and NO3 ions. All spectroscopic measurements were studied in a mixed solvent system of acetonitrile and water (CH3CN[thin space (1/6-em)]:[thin space (1/6-em)]H2O = 6[thin space (1/6-em)]:[thin space (1/6-em)]4, v/v) mixture.

In the absorption spectrum the probe BTA exhibited a prominent red shift (∼15 nm) exclusively for Hg2+ ions, while other tested cations (Fig. 1a) and anions (Fig. S7) induce negligible changes, suggesting a target specific recognition. These observations clearly validate the selective recognition of Hg2+ ions by probe BTA, whereas other cations (Fig. 1b) and anions (Fig. S7b) failed to produce any comparable fluorescence variations (Fig. 1f). To acquire deeper understanding into the interaction mechanism, UV-vis titration experiments were performed by gradually increasing the concentration of Hg2+ ions. The absorbance spectrum of BTA exhibited an intense absorption band centered at 325 nm, which progressively decreased in intensity with increasing concentration of Hg2+ ions. Simultaneously, a new absorption band appeared at 340 nm, accompanied by the emergence of an isosbestic point at 335 nm (Fig. 1c). The presence of the isosbestic point indicates a well-defined equilibrium between the BTA and BTA–Hg2+ complex. Fluorescence titration experiments provided further evidence for this interaction. As presented in Fig. 1d, a substantial enhancement in emission intensity at 418 nm was observed upon the progressive addition of Hg2+ ions (Fig. S8), reaching saturation after the introduction of one equivalent of Hg2+ ions. The other metal ions did not induce any notable emission responses, highlighting its excellent specificity of probe BTA towards Hg2+ ions. The linear relationship between fluorescence intensity and Hg2+ concentration exhibited an excellent correlation (R2 = 0.99529), from which the detection limit was estimated to be 114 nM, demonstrating the high sensitivity of BTA for Hg2+ ions detection. The observed enhancement in emission intensity can be attributed to the restriction of photo induced electron transfer (PET) or suppression of non-radiative decay processes upon coordination with Hg2+.34


image file: d6ra03004a-f1.tif
Fig. 1 (a) UV-vis absorption spectra and (b) fluorescence spectra of probe BTA (20 µM) in (CH3CN[thin space (1/6-em)]:[thin space (1/6-em)]H2O) (6[thin space (1/6-em)]:[thin space (1/6-em)]4, v/v) solution in response to 1 mM of diverse metal cations (5 equiv.). Variation of (c) UV-vis absorption spectra and (d) emission spectra of probe BTA in the presence of increasing concentration of Hg2+ ions (0–2 equiv.) inset: linear response curve of BTA depending on the various concentration of Hg2+ ions. (e) Competition experiments of BMA (20 µM) toward Hg2+ ions in the presence of 10 mM of other metal ions in CH3CN/H2O (6[thin space (1/6-em)]:[thin space (1/6-em)]4, v/v). (f) Photograph of probe BTA before and after addition of metal ions under UV region.

The fluorescence quantum yield was determined using anthracene as a reference with a known ϕR of 0.27 in ethanol. The calculated quantum yield values were 0.022 for BTA, and 0.043 for BTA–Hg2+ complex. These results clearly indicate an enhancement in fluorescence intensity upon binding of BTA with Hg2+ ions.

To confirm the anti-interference capability of probe, competitive fluorescence studies were performed in the presence of different coexisting metal cations (Fig. 1e and S9a) and mixed ions (Fig. S9b). The emission response of BTA to Hg2+ remained unaffected, even under competitive conditions, confirming its robust selectivity. Collectively, these results demonstrate that BTA severs as a highly selective and sensitive fluorescent ON chemoprobe for the detection of Hg2+ ions with clear optical transitions and strong resistance towards various interfering metal species in a mixed solvent system.

Elucidation of binding stoichiometry and sensing mechanism of BTA

Based on the spectroscopic outcomes, the plausible sensing mechanism for the coordination of probe BTA to Hg2+ is proposed. Upon coordination with Hg2+ ions, probe BTA displays a fluorescence turn-on signal owing to target specific interaction of Hg2+ with the donors of nitrogen and sulfur atoms present in 4-(bis(2-((4,5-dihydrothiazol-2-yl)thio)ethyl)amino)benzaldehyde moiety.

To validate this proposed sensing mechanism, Job plot, NMR titration, FT-IR and HR-MS studies were systematically performed. The Job's plot analysis revealed the formation of a 1[thin space (1/6-em)]:[thin space (1/6-em)]1 binding stoichiometric adduct between BTA and Hg2+ (Fig. S10). This observation was further corroborated by HR-MS analysis (Fig. S11). In the mass spectrum the peak at m/z value of 839.5945 corresponding to [BTA + Hg2+ + 2H2O], corroborating the proposed complexation stoichiometry. The Kd value for Hg(II) was 5.4 nM (R2 = 0.99) (Fig. S12).

To acquire deeper insight into the binding interaction, 1H NMR titration experiment was performed in DMSO-d6 solvent. Fig. 2 displays the configurations of protons in BTA after interaction with Hg2+ ions. The resonance signals observed in the region of 3.26–4.26 ppm correspond to the aliphatic protons of BTA. The proton signals at 7.03–7.05 (Hb) and 7.90–7.92 (Hc) ppm are assigned to the aromatic protons of binding unit. While the biphenyl aromatic protons appear as merged signals at 7.56–7.22 ppm. Nevertheless, following addition of Hg2+ ions, the peak of Ha proton at the aliphatic region undergoes a slight shift from 3.66–3.68 ppm. Due to the geometrical coordination the aromatic protons of and Hb and Hc a small downfield shift to 7.91–7.94 ppm and 7.06–7.08 ppm. Furthermore, the biphenyl aromatic proton signals at the region 7.55–7.28 ppm displayed clear splitting. These spectral perturbations strongly suggest that the nitrogen and sulfur atoms of the thiazoline moiety and the nitrogen on the phenylamine serve as the primary binding sites for Hg2+ ions.


image file: d6ra03004a-f2.tif
Fig. 2 1H NMR titration of probe BTA with Hg2+ (0–2 eq.) in DMSO-d6. (a) Aliphatic region; (b) aromatic region. (c) Proposed reaction mechanism for probe BTA with Hg2+ ions.

The FT-IR spectra of BTA in the absence and presence of Hg2+ were recorded and are shown in Fig. S13. For BTA, the absorption bands observed at 956, 1134, 1284, and 1566 cm−1 correspond to C–C stretching, C–N stretching, C–N (ring stretching), and C[double bond, length as m-dash]N stretching, respectively. Upon coordination with Hg2+, the FT-IR spectrum of BTA–Hg2+ exhibits significant band broadening and partial merging of these characteristic vibrations, particularly in the C–N/C–C regions, while the C[double bond, length as m-dash]N stretching band disappears. These spectral changes indicate a strong interaction between Hg2+ ions and the receptor unit of BTA, confirming the involvement of heteroatoms in metal coordination (Fig. 2c).

Evaluation of the reversible, kinetic, and logical sensing functions of BTA

Reversibility is an important criterion for estimating the practical applicability of a fluorescent sensor. The reversible sensing behaviour of the probe BTA to Hg2+ ions were studied in a binary solvent system (CH3CN[thin space (1/6-em)]:[thin space (1/6-em)]H2O = 6[thin space (1/6-em)]:[thin space (1/6-em)]4, v/v) using KI as a regenerating agent. The probe BTA displayed nominal emission centered at 413 nm. Upon interacting with Hg2+ ions, the emission intensity increased at 418 nm, indicating complex formation between BTA and Hg2+ ions, following addition of potassium iodide (KI) decreased the fluorescence to the original level of BTA signal (Video S1), which confirms the restoration of free probe BTA.

Upon alternative addition of Hg2+ and KI demonstrated a clear OFF–ON–OFF switching pattern of the reversible fluorescence phenomenon. The fluorescence response remained constant over five successive cycles, demonstrating the repeatability of the probe BTA (Fig. 3a). These observations confirm the excellent reversibility and regeneration capability of BTA, an essential attribute for reusable sensing applications.


image file: d6ra03004a-f3.tif
Fig. 3 (a) Change in fluorescence of BTA after the sequential addition of Hg2+ and KI. (b) The time-dependent fluorescence spectra of BTA–Hg2+ complex. (c) Logic representation of molecular AND gate; Truth table of AND gate; bar diagram of AND gate for Hg2+ ions and other metal ions.

To further authenticate the sensing performance, the response kinetics of BTA towards Hg2+ ions were examined using time-resolved fluorescence spectroscopy. Time-dependent fluorescence measurements showed that the emission intensity at 418 nm of BTA reached its maximum within 4 seconds after the addition of Hg2+ (Video S2), after which it remained constant without further variation in emission intensity. This rapid response towards Hg2+ ions, demonstrates its potential for real-time monitoring of mercury contamination (Fig. 3b).

In addition to its reversible and rapid response characteristics, this system was also explored for its molecular logic gate functionality. Inspired by the growing interest in molecular systems capable of mimicking digital operations, the fluorescence modulation of BTA was employed to design a molecular AND logic gate (Fig. 3c). In this logical framework, BTA, Hg2+, and various metal ions (M+) were assigned as chemical inputs, while the emission intensity at 418 nm (I418) was assigned as the optical output. The output followed a binary threshold: I418 > 1000 corresponds to “1” (ON) and ≤1000 to “0” (OFF). Only when both BTA and Hg2+ were present, the system exhibits strong fluorescence, producing an output of “1,” thus satisfying the AND gate logic. Other metal ions failed to activate fluorescence enhancement, yielding a “0” output corresponding to the OFF state.

Thus, the probe BTA efficiently functions as a molecular AND logic gate, combining selective Hg2+ recognition with an intelligent optical signal processing.

Quantum chemical investigations of BTA

To gain better insight into the photophysical behaviour of the probe BTA and its complex with Hg2+ ions, density functional theory (DFT) calculations were performed using Gaussian 09. Geometry optimizations of the free probe BTA were performed at the B3LYP/6-31G (d,p) level, whereas the B3LYP/LANL2DZ basis set was used for the BTA–Hg2+ complex. The Frontier Molecular Orbitals (FMOs) of BTA and its metal complex are displayed in Fig. 4. In the free BTA molecule, the HOMO electron density is primarily localized over the diphenyl unit and recognition moiety, while the LUMO electron density is located over the 2 thiazoline thiol parts. In contrast, for the BTA–Hg2+ complex, the electron density of HOMO was distributed over receptor region, but the LUMO becomes predominantly localized on Hg2+. This redistribution of electron density upon Hg2+ coordination supports a photoinduced electron transfer (PET) mechanism as the basis of fluorescence enhancement.35 The calculated HOMO–LUMO energy gaps for BTA and BTA–Hg2+ are 3.91 eV and 2.36 eV, respectively. The reduction in energy gap upon complexation indicates enhanced electronic delocalization and the formation of a more stable complex, which corroborates well with the experimentally observed fluorescence “ON” response of BTA toward Hg2+ ions.
image file: d6ra03004a-f4.tif
Fig. 4 Frontier molecular orbital (FMOs) of the BTA and the BTA–Hg2+ complex.

Solid-state sensing application of BTA–PVA film

The development of solid-state sensing materials based on polymers has become important for environmental and biological monitoring, predominantly for the recognition of hazardous ions. Among such materials, polyvinyl alcohol (PVA) films have emerged as a best platform owing to their optical transparency, mechanical flexibility, chemical stability, and their capability to uniform immobilization of ligands.36,37

2 g of PVA was dissolved in 20 mL of deionized water and heated to 90 °C for 3 h to obtain a uniform solution. Once cooled to room temperature, 2 mL of BTA solution (0.02 g mL−1) was introduced, followed by further stirring for 1 hour. The resulting solution was poured into a clean Petri dish and left to dry under ambient conditions for about 48 hours.38 The dried BTA/PVA (2 wt%) film was then carefully peeled off and cut into the required shapes (Fig. 5a). The film exhibited weak blue fluorescence under UV region, making it suitable for the detection of Hg2+ ions via fluorescence “turn-on” response. The emission spectra exposed that, although the BTA/PVA film displayed moderate emission, a striking enhancement in fluorescence intensity at 395 nm was observed only for Hg2+ ions (Fig. 5b). On the other hand, only slight changes in emission intensity were observed for tested various cations, emphasizing the remarkable selectivity of the BTA/PVA film. In addition, a quantitative analysis for BTA/PVA film was carried out using Hg2+ ions, upon increasing the concentration of Hg2+ ions, the fluorescence intensity was increased progressively, which was correlated with the life time measurements (Fig S15). The turn-on response toward Hg2+ ions is due to favourable binding interactions that restrict non-radiative decay.


image file: d6ra03004a-f5.tif
Fig. 5 (a) Fabrication of BTA/PVA film; (b) fluorescence spectra of solid-state detection of mercury ions using PVA/BTA.

Overall, this matrix-assisted emission enhancement, combined with the film's stability and simplicity, shows that BTA/PVA is a highly promising material for practical solid-state mercury monitoring applications.

Comparison with other chemosensors

The advanced sensing performance of the probe BTA was assessed with previously reported mercury sensors (Table S1). BTA displays several distinct advantages, such as noticeable fluorescence turn-on response, robust anti-interference ability, excellent reversible behaviour, and rapid reaction kinetics. Furthermore, the successful incorporation of BTA into PVA films demonstrates the possibility for practical and on-site mercury detection. Collectively, these features make BTA as a highly promising material for environmental monitoring and remediation applications.

Conclusion

In conclusion, by engineering an imidazole-based ligand, we developed a fluorescent chemosensor (BTA) for the selective and sensitive detection of Hg2+ ions. The chemoprobe BTA displayed a prominent emission enhancement upon interaction with Hg2+ ions, with the detection limit of 114 nM. The plausible binding mechanism between BTA and Hg2+ ions was systematically interpreted through UV-vis and fluorometric titrations, NMR spectroscopy, HR-MS, and FT-IR analysis, in addition DFT calculations provided theoretical authentication for the proposed sensing mechanism. Additionally, the practical applicability of the chemoprobe BTA was demonstrated by its successful utilization in PVA film-based detection, highlighting its potential for real-world environmental monitoring.

Author contributions

Bharathkumar Thangaraj: conceptualization, writing original draft; Suresh Ranganathan: data curation, methodology; Lakshmipriya Kannan: formal analysis, writing – review & editing; Karthikeyan Natesan Sundaramurthy: supervision, validation; Ravichandran Cingaram: project administration, resources; Sathiyanarayanan Kulathu Iyer: project administration, resources.

Conflicts of interest

There are no conflicts to declare.

Data availability

Data will be made available on request.

Supplementary information (SI): characterization data, photophysical studies, and additional spectra and figures supporting the findings of this work. See DOI: https://doi.org/10.1039/d6ra03004a.

Acknowledgements

NSK acknowledges the DST – SERB for Young Scientist Scheme Project (Ref. No. SB/FT/CS-067/201S), Atomic Energy Regulatory Board, India for sanctioning the CSRP project (Ref. No. AERB/CSRP/PROJ. No. 65/06/2017), and the Grand-in-Aid by FIST scheme from Department of Science and Technology, India (SR/FIST/college-110/2017).

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