Open Access Article
Tingting Zhang,
Juan Zhang,
Yanyan Li,
Caiyuan Guo,
Yuehua Liang,
Jiuzhi Wei,
Xinxian Ma
* and
Xinning Han*
Ningxia Key Laboratory of Green Catalytic Materials and Technology, College of Chemistry and Chemical Engineering, Ningxia Normal University, Guyuan 756099, China. E-mail: maxinxian@163.com
First published on 6th October 2025
In this study we developed white light-emitting gel materials based on two mechanisms, namely, acid-induced protonation and Förster resonance energy transfer (FRET), and applied them to information protection and encryption. The newly synthesized compound, Q, forms different protonation states after protonation, and the multicolor emissions from these states ultimately achieve white-light emission through spectral superposition. When Q is paired with dyes such as Nile red, rhodamine 6G, and acridine red, it can act as an energy donor in the FRET system, enabling white-light emission at a specific, optimized ratio. Two functional gels based on polyvinyl alcohol (PVA) were developed, namely a PVA–Q–Nile red composite material and a PVA–Q–H+ (150 eq. H+ to Q) responsive gel. These gels exhibit stable white light emission properties and can be used for writing and encrypting high-resolution information. Additionally, the PVA–Q–H+ responsive gel possesses time-dependent encryption functionality: triggered by OH−, the written traces can realize controllable self-erasure. The gel material developed in this study based on a white-light emission system with dual-responsive mechanisms provides a novel strategy for the design and synthesis of intelligent anti-counterfeiting materials.
At present, the main strategies for constructing WLE materials include single-molecule systems,7 supramolecular assemblies,8,9 metal–organic frameworks,10 and energy transfer mechanisms based on fluorescence resonance energy transfer (FRET).11 These strategies have been successfully applied to the preparation of WLE gels. Notably, gel materials, due to their high tunability, provide flexibility for customized information encryption and have been widely applied in anti-counterfeiting fields such as food safety and 3D anti-counterfeiting printing.12–15 Although gels with excellent stability can be prepared based on single-molecule white-light emission systems,16 these systems pose significant challenges in molecular design.17 For instance, Liang et al.18 designed a single-molecule WLE hydrogel through dual acid–base channel regulation, enabling time-dependent and water vapor-responsive information encryption; Wang et al.19 developed a thermo-responsive hydrogel that achieved dynamic WLE by regulating the protonation equilibrium of fluorophores via temperature control. However, such regulation mechanisms relying on a single external stimulus have inherent limitations: their emission colors are indirectly adjusted by altering the microenvironment of the polymer, and combined with the thermal hysteresis characteristics of hydrogels, it is difficult to maintain the WLE state accurately and stably.
Beyond single-molecule systems, FRET is also a critical mechanism for achieving WLE. This provides another important pathway for realizing efficient and tunable WLE. Its effective operation requires the fulfillment of three core conditions: (i) the donor–acceptor distance is maintained within the range of 1–10 nanometers; (ii) the emission spectrum of the donor sufficiently overlaps with the absorption spectrum of the acceptor; and (iii) the spatial arrangement of donor–acceptor transition dipoles is appropriate.20–23 FRET assisted white-light emission serves as a remarkably concise and advanced function in high-level anti-counterfeiting.24 For example, Ma et al.25 developed a WLE hydrogel with both information protection writing and alkaline gas detection capabilities; Mardani et al.26 regulated white-light emission WLE by adjusting the efficiency of FRET through temperature and pH, and this approach has been widely applied. This provides insights for the design of multi-responsive information encryption materials.
Based on the above research, it has been observed that most current organic WLE systems either rely on a single modulation mechanism or suffer from complexity and uncontrollability caused by the introduction of multi-mechanism coupling. Therefore, significant challenges are faced in meeting the comprehensive requirements for the flexibility and precision of luminescence regulation in the field of information encryption, which makes the development of novel multiple pathways and mechanism regulation systems an urgent need. To address the aforementioned issues, this study innovatively proposes a dual-responsive WLE system. Its core advantage lies in providing two parallel and completely independent regulation channels for achieving stable and reversible white-light emission: the first is an acid-induced intramolecular protonation channel, and the second is an intermolecular FRET energy transfer channel. Compared with existing systems, this design not only overcomes the dependence on a single external stimulus, but also avoids the complexity and uncontrollability caused by multi-mechanism coupling, thereby significantly improving the regulation precision and operational flexibility of white-light emission.
Specifically, a new fluorescent compound, Q (Scheme 1), was designed and synthesized, and its luminescence properties were verified with time-dependent density functional theory (TD-DFT) calculations. This molecule can generate white light either through acid-induced intramolecular protonation or through intermolecular FRET processes with acridine red, rhodamine 6G (Rh6G), and Nile red. Furthermore, two multifunctional gels, PVA–Q–Nile red and PVA–Q–H+ (150 eq. H+ to Q), were prepared using polyvinyl alcohol (PVA) as the matrix. Both gels are capable of information writing and encryption. Among them, the time-varying properties of the PVA–Q–H+ gel enable automatic information erasure through the action of OH−, effectively preventing the risk of secondary leakage and providing a new direction for the research and development of information encryption materials (Fig. 1).
Proton nuclear magnetic resonance (1H NMR; 400 MHz) and 13C NMR (101 MHz) spectroscopic analyses were performed using a 400 MHz Bruker spectrometer. A Shimadzu RF-6000 fluorescence spectrophotometer was used to obtain the fluorescence spectra. Mass spectrometry was performed using an Autoflex Speed TOF/TOF. Fourier transform infrared (FT-IR) spectra of the samples were obtained using an IR spectro-photometer (Thermo Scientific Nicolet iS5) in a wavenumber range of 400–4000 cm−1. The quantum yields (QYs) were determined using an Edinburgh FLS1000 instrument. A Shimadzu UV-1750 spectrometer was used to record the ultraviolet-visible (UV-vis) absorption spectra of the samples. The fluorescence lifetimes were recorded with a time-correlated single-photon counting spectrometer (Edinburgh FLS1000). Quantum chemistry calculations were performed at the PBE0/6-311G* level of theory based on TD-DFT using Gaussian 09 software.
:
1 ([Q] = 1 × 10−3 mol L−1). The mixture was heated and stirred at 100° C for 6 h, then poured into a Petri dish and refrigerated at −10° C for 12 h. After taking it out and thawing, a white fluorescent PVA–Q–Nile red gel was obtained.
:
1 ([Q] = 1 × 10−3 mol L−1). The mixture was heated and stirred at 100° C for 6 h, then poured into a Petri dish and refrigerated at −10° C for 12 h. After taking it out and thawing, a white fluorescent PVA–Q–H+ gel was obtained.
First, the geometric configuration of the solvated system was optimized using the hybrid functional PBE0/6-311G* basis set. Subsequently, by optimizing the first singlet excited state (S1) structure of Q in DMSO, we obtained the S0 → S1 excitation energy and corresponding molecular orbital diagrams (Fig. 2a). The fluorescence emission spectrum was then simulated using the Multiwfn program, yielding a calculated emission wavelength of 512 nm for Q.28 Experimentally, the emission maximum of Q in DMSO solution was measured at 522 nm (Fig. 2b), demonstrating excellent consistency with the theoretical prediction. Furthermore, the excitation and emission spectra of Q were experimentally recorded (Fig. 2c), with follow-up measurements performed using a fixed excitation wavelength of 422 nm for photophysical characterization.
Fig. 4b and S11 show the considerable evolution of the emission spectra of Q in DMSO solution upon gradual addition of H+: the overall fluorescence intensity progressively decreased, with marked attenuation of the red (∼620 nm) and green (∼550 nm) emission components, while the blue component (∼450 nm) exhibited relative enhancement. When the H+ concentration reached 150 eq., the system achieved white-light emission. Fig. 4a, c, e and f show the systematic color changes of the fluorescent solution with an increase of H+ concentration (0–150 eq.): initial green (0 eq.) → yellow-green (5 eq.) → yellow-white (60 eq.) → white light (150 eq.). At 150 eq. H+, the CIE coordinates are (0.29, 0.33), which is very close to the pure white light emission with chromaticity coordinates (0.33, 0.33) in the 1931 Commission Internationale de l’Éclairage (CIE) standard chromaticity system.30 The observed phenomenon likely stems from distinct fluorescence emissions generated by different protonation states of Q, with spectral superposition of these multicolor emissions governing white-light generation.
To analyze the H+-induced structural modification, we conducted 1H NMR (Fig. S12 and S13) spectroscopy analysis in combination with the ESP of molecule Q (Fig. 4d). During the gradual addition of H+ to the DMSO-d6 solution of Q, the nitrogen atom on the imidazole ring was found to be preferentially protonated. After protonation, the electron cloud density of the imidazole ring system decreased significantly, resulting in a strong deshielding effect. This deshielding effect caused the proton peak of N–H on the imidazole ring and the proton peak of C–H (δ = 8.2 ppm) on the adjacent benzene ring to shift to the low field. With the continuous addition of H+, the C
N bond in the hydrazone structure underwent protonation. Similarly, due to the deshielding effect, the signal peak of C–H at 7.9 ppm on the adjacent benzene ring also shifted to the low field. The absence of a significant change in the C–H signal peak at 7.0 ppm indicated that the –OH group was not protonated. The signal peaks of N–H and –OH in the hydrazone structure weakened or even disappeared because the acidic environment accelerated the proton exchange rate. The shift of the C–H signal peak at 7.3–7.5 ppm to the low field might be attributed to the protonation of Q, which reduced the electron cloud density and electronegativity while enhancing the deshielding effect, thereby causing rotation of some structures in the molecule. The structure of molecule Q after protonation is shown in Fig. S14. This redistribution of electrons modulates the π-conjugated system, ultimately affecting the luminescence properties. When the concentration of H+ reached 150 eq., almost all free Q molecules in the solution were converted into substances in different protonation states. The luminescence superposition effect of these different protonated forms is the fundamental reason for the generation of white-light emission.
Subsequently, UV-vis spectroscopy (Fig. S15) was employed to analyze the protonation process of Q in DMSO. Consistent with the NMR observations, a distinct hypsochromic shift of 10 nm (from 361 to 351 nm) in the characteristic absorption peaks was observed during progressive protonation, with the spectra showing no further changes upon reaching the saturated protonation state.
Finally, FT-IR spectroscopy (Fig. S16) confirmed the interaction between Q and H+ after the addition of 150 eq. H+. The carbonyl stretching vibration of pristine Q at 1648 cm−1 exhibited a bathochromic shift to 1633 cm−1 upon protonation, providing direct evidence of Q–H+ interactions.
As shown in Fig. 5a, Q in DMSO exhibits a strong fluorescence emission peak at 522 nm, with an emission band spanning 400–750 nm. In contrast, Nile red in DMSO displays a maximum absorption peak at 545 nm, covering an absorption range of 400–640 nm, demonstrating the best spectral overlap with Q's emission. Although the Q–Nile red system exhibits relatively weak overall emission intensity (Table S1), white-light emission is achieved at a molar ratio of 50
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1 (Nile red
:
Q) under 422 nm excitation, with CIE coordinates of (0.34, 0.38), closely approaching the pure white-light reference point (0.33, 0.33). As shown in Fig. 5c, upon excitation at 422 nm, gradual addition of Nile red to a 1 × 10−3 M solution of Q in DMSO resulted in a systematic decrease in the fluorescence intensity of Q at 522 nm, accompanied by the emergence of a new emission band at 630 nm. Concurrently, the fluorescence intensity of Nile red progressively increased, reaching its maximum at a Q-to-Nile red molar ratio of 10
:
1. Comparative analysis of the fluorescence emission profiles between the Q–Nile red system (10
:
1 molar ratio) and pure Nile red confirmed the occurrence of FRET. Notably, under 422 nm excitation, pure Nile red exhibited weak fluorescence intensity, and increasing its concentration did not enhance emission. The observed intensity increase at 630 nm is attributed to efficient energy transfer from Q to Nile red. The fluorescence quantum yield of the Q–Nile red system and pure Q were 40.1% and 58.1%, (Fig. S21). Subsequently, the fluorescence decay experiment showed that the lifetimes decreased from the Q (τ = 2.29 ns) system to the Q−Nile red system (τ = 2.16 ns) (Fig. S20), indicating that the energy harvested by Q had been successfully transferred to Nile red.
:
1 (Q
:
Nile red). The resulting mixture was heated and stirred at 100 °C for 6 hours, after which it was poured into a Petri dish and refrigerated at −10 °C for 12 hours. After removal and thawing, the PVA–Q–Nile red gel with white fluorescence was obtained. The chromaticity coordinates of its white light emission were (0.32, 0.34) (Fig. S17a), which were closer to the ideal white point (0.33, 0.33) compared with the DMSO solution of Q and Nile red. This phenomenon is presumably attributed to the selective absorption of red light in the system by the PVA gel matrix. Considering that Q can emit green fluorescence with low intensity in the presence of an alkali, we used an aqueous OH− solution to write on the as-prepared gel (Fig. S23). No obvious writing traces were observed on the gel under natural light; however, distinct writing traces became visible under a 442 nm UV lamp. Owing to this unique property, the PVA–Q–Nile red gel can serve as a dedicated writing material to realize the protection and encryption of information.
Subsequently, using the same matrix preparation method, we further synthesized the PVA–Q–H+ white fluorescent gel (Fig. 6a). Intermolecular hydrogen bonds may have been formed between PVA and molecule Q through cross-linking interactions (Fig. S24).31 These hydrogen bond interactions can effectively restrict the free movement of Q molecules but do not affect the migration of H+. We used an aqueous OH− solution to write on the surface of the PVA–Q–H+ gel (Fig. 6b and c). When the gel surface came into contact with OH−, a deprotonation reaction occurred, forming a distinct green fluorescent region. As time elapsed, the written traces showing green fluorescence gradually faded and completely disappeared after 60 minutes, with the written region reverting to the initial white fluorescence. This information “self-erasing” phenomenon is presumably due to the fact that the H+ concentration inside the gel is higher than that of the externally introduced OH−. When the OH− on the surface of the gel is completely consumed, since H+ can migrate freely within the gel, the depleted H+ in the system is replenished over time, causing the Q molecules in the writing area to be protonated again, and the fluorescence will return to white. Based on this unique time-responsive property, we have developed a white-light information encryption material with time dependence.
To evaluate the structural stability of the two gels in practical applications, we further tested the elastic moduli of the PVA–Q–H+ gel and the PVA–Q–Nile red gel (Fig. S25). The results showed that the PVA–Q–Nile red gel had an elastic modulus of 50 kPa, and this relatively high value indicates strong rigidity and resistance to deformation under an external force. In contrast, the PVA–Q–H+ gel had an elastic modulus of 5 kPa, and this lower value confers weaker rigidity but greater flexibility, allowing it to deform easily under a force while maintaining good recovery ability. To verify the influence of mechanical properties on fluorescence performance, we conducted twist deformation tests on the two gels (Fig. S26), and no obvious change in their fluorescence colors was observed, demonstrating the stability of their fluorescence performance under mechanical deformation.
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