Yoonjae Choi,
Myeongjin Kang and
Song-Ho Byeon*
Department of Applied Chemistry, College of Applied Science and Institute of Natural Sciences, Kyung Hee University, Gyeonggi 17104, South Korea. E-mail: shbyun@khu.ac.kr
First published on 29th January 2025
Nicotinic acid (NA; also known as niacin or vitamin B3), an essential nutrient for humans, was inserted into the interlayer spaces of Eu3+-doped layered yttrium hydroxide (LYH:Eu). This hybrid system, NA-LYH:Eu, demonstrated remarkable efficiency in the storage of NA, offering long-term stability, reusability, and controlled, sustained release capabilities. Notably, the intercalated NA sensitized the luminescence of Eu3+ ions via the transfer of UV-energy absorbed for its π → π* transition from the S0 ground state to the S1 excited state, leading to the characteristic 5D0 → 7FJ (J = 1–4) transitions. The resulting bright red emission could be reversibly quenched and restored through repeated NA release (chloride uptake) and re-inclusion cycles within the LYH:Eu interlayers, demonstrating the potential application as a chloride-induced corrosion inhibitor. The release rate of NA in a phosphate buffer solution could be modulated by tuning the crystallinity and particle size of the LYH:Eu host. When highly crystalline NA-LYH:Eu was employed, the in vitro release of NA continued beyond 5 days without reaching equilibrium. Concurrently, the red emission from a colloidal solution containing NA-LYH:Eu particles gradually diminished as the release progressed, providing a visually observable indicator. This luminescence ‘on/off’ behavior offers a practical method for in situ visual monitoring of NA inclusion and release.
NA also exhibits catalytic properties due to its potential Lewis base (pyridine ring) and Brønsted acid (carboxyl group) functionalities.7 These characteristics enable its use as an organocatalyst, where immobilization on silica extends its functionality from homogeneous to reusable heterogeneous catalytic conditions for organic synthesis.8 Moreover, NA serves as a bridging ligand in metal–organic frameworks (MOFs), enhancing therapeutic efficacy through synergistic effects.9 The strong coordination ability of NA-related acids has also been utilized to immobilize lanthanide complexes in organic–inorganic hybrid materials, where the carboxyl group moderates reactivity toward hydrolysis and condensation and the pyridine ring coordinates with lanthanide ions, sensitizing their luminescence.10–12 Additionally, NA has demonstrated anti-corrosion effects on steel by forming a protective layer on γ-FeOOH surfaces and isolating the substrate from corrosive agents.13
In recent years, encapsulating organic molecules within inorganic matrices has emerged as an effective strategy to overcome their limitations under conventional conditions. These organic–inorganic hybrids have been utilized as delivery systems for therapeutic drugs, genes, cosmetic ingredients, and composite materials in polymeric matrices.14–17 Layered double hydroxides (LDHs) are prominent examples of inorganic matrices capable of releasing organic anions in a controlled and sustained manner.18 The positively charged layers of LDHs and their ion exchange capacity allow them to accommodate anionic molecules, including organic carboxylates.19,20 NA, a member of the pyridinecarboxylic acid group, can also be readily intercalated into the interlayer of LDHs to form NA-LDH hybrids. This characteristic can be applied to separate NA, which is discharged into wastewater systems each year, from aqueous solutions.21 The interlayer space of LDHs provides NA with significantly enhanced chemical, thermal, and photostabilities, as well as control and sustainability in its release. For instance, NA-LDH hybrids have been explored for sustained release in topical applications,22 as corrosion inhibitors in coastal construction,23 and for their organocatalytic selectivity and recyclability. However, high NA concentrations can disrupt the LDH layered structure, limiting its loading capacity.24
Recently, layered rare-earth hydroxides (LRHs) have gained attention as alternative inorganic matrices for organic–inorganic hybrid systems. Similar to LDHs, LRHs have a lamellar structure consisting of hydroxocation layers alternated with charge-compensating anion layers. Their general formula is represented as [RE2(OH)5·nH2O]+(Xm−)1/m (RE = rare earth elements, X = interlayer anions).25 LRHs are known for their ease of preparation, anion exchange capability, and high stability under varying pH and pressure conditions, making them suitable for applications such as bioimaging and environmental adsorption.26,27 Furthermore, the optical properties of RE ions in LRH layers have shown great potential for luminescent delivery systems of bioactive molecules.28–30 In this study, Eu3+-doped layered yttrium hydroxide (LYH:Eu) was investigated as a matrix for the efficient loading and sustained release of NA. Notably, interlayer NA ions acted as ‘antenna molecules’, effectively sensitizing Eu3+ luminescence. This luminescent ‘on/off’ behavior enabled real-time probing of NA inclusion and release within the interlayer spaces of LYH:Eu.
Fig. 1a shows the XRD pattern of the prepared LYH:Eu host. The series of strong and sharp (00l) reflections indicate a well-crystallized typical layered structure. Variations in reaction time, HMT concentration, and/or solution temperature during synthesis led to noticeable differences in the crystallinity and particle size of LYH:Eu. The observed average interlayer distance, approximately 9.2 Å, is consistent with previously reported values for LYH (9.18 Å).31 Minor discrepancies could be attributed to Eu3+ doping within the LYH layers and variability in the amount of interlayer water. The experimental molar ratio determined by ICP analysis, Y:
Eu = 0.903(1)
:
0.104(2), was close to the nominal composition of LYH:Eu. Fig. 2a presents the TGA curve of LYH:Eu, which reveals three distinct weight-loss events. These are centered at approximately 100 °C, 300 °C, and 520 °C and correspond to the loss of surface and interlayer water, the dehydroxylation of hydroxide layers, and the decomposition of nitrate anions to form Y2O3:Eu.32 The total observed weight loss of 36.2% is in close agreement with the calculated value of 36.17%, corresponding to the thermal decomposition of Y1.8Eu0.2(OH)5NO3·2.0H2O leaving Y1.8Eu0.2O3. The FT-IR spectra of LYH:Eu are displayed in Fig. S1a (ESI†). Broad peaks observed at approximately 3300–3500 cm−1 and 1638 cm−1 are assigned to the stretching and bending modes of hydroxyl groups and interlayer water molecules, respectively. The strong band at around 1380 cm−1 corresponds to the asymmetric stretching (ν3) mode of nitrate within the interlayer space.33
As shown in Fig. 1b, the strong (00l) reflections in the XRD pattern of NA-LYH:Eu confirmed the preservation of the typical layered structure after the reaction between LYH:Eu and aqueous NA. A systematic shift of (00l) reflections to lower angles, corresponding to an increased interlayer distance from 9.2 Å to approximately 14.7 Å, was observed, indicating the successful replacement of nitrate by NA anions. The TGA curves of NA-LYH:Eu and pure nicotinic acid, compared with LYH:Eu, are shown in Fig. 2. NA-LYH:Eu exhibited three main weight-loss steps (Fig. 2b). The initial weight loss below 100 °C was attributed to the evaporation of water. For comparison, pure nicotinic acid decomposed completely in a single-step process below 230 °C (Fig. 2c). A slight weight loss in NA-LYH:Eu centered at similar temperature range likely resulted from the removal of NA molecules adsorbed on the particle surface. The dehydroxylation of NA-LYH:Eu layers occurred at around 270 °C, slightly lower than that of pristine LYH:Eu, while the decomposition of interlayer NA began at approximately 420 °C. Thus, the interlayer environment provided by LYH:Eu enhanced the thermal stability of NA through electrostatic attractions and effective intermolecular interactions, protecting the interlayer NA. This thermal stability suggests that the hybrid material could mitigate the loss of thermally unstable nicotinic acid (vitamin B3) during high-temperature food processing.6 The amounts of interlayer water and surface-adsorbed NA were determined based on weight losses at approximately 100 °C (7.3%) and 190 °C (3.2%), respectively. Considering that Y2O3:Eu oxide was obtained after thermal decomposition of NA-LYH:Eu at 1000 °C, the chemical formular could be determined by the total weight loss, including interlayer water evaporation, layer dehydroxylation, and interlayer NA decomposition. Thus, the observed total weight loss of 45.2% closely matched the calculated value of 45.8% for Y1.8Eu0.2(OH)5(interlayer NA)(surface NA)0.1·1.7H2O. This agreement suggests nearly complete replacement of nitrate by NA anions. The NA loading capacity in LYH:Eu, measured as approximately 305 mg g−1, exceeded previously reported capacities in Zn/Al LDHs with similar structures.22 This high loading capacity highlights the potential of LYH as an effective reservoir or carrier for NA. Fig. S1b (ESI†) compares the FT-IR spectra of NA-LYH:Eu and LYH:Eu host, showing significant differences. The appearance of strong bands at approximately 1560 cm−1 and 1392 cm−1, corresponding to the antisymmetric (νas) and symmetric (νs) stretching vibrations of –COO− groups, respectively, confirmed the presence of interlayer NA after the exchange reaction. Additionally, a strong band at approximately 1606 cm−1 was attributed to the C–C stretching vibration (νC–C) of the pyridine ring.35 In general, the CO stretching band of the –COOH group in free acids appears around ∼1690 cm−1 in their spectra. Therefore, the shoulder observed in a similar region in the NA-LYH:Eu spectrum supports the presence of free nicotinic acid adsorbed on the surface.
Subtracting the layer thickness of 6.5 Å from the observed interlayer distance of 14.7 Å for NA-LYH:Eu suggests an available gallery height of approximately 8.2 Å for interlayer anions.36 This height, significantly larger than the molecular length (∼6.5 Å) of NA, which has a planar structure with a pyridine ring and a carboxyl group, implies that NA anions are arranged in a partially interdigitated bilayer mode within the interlayer space. Similar to the arrangement of interlayer benzoate anions,37 the carboxyl groups alternate in orientation toward adjacent hydroxide layers to form hydrogen bonds, while the pyridine rings are centrally positioned within the interlayer space, facilitating effective π–π stacking. A long-range hydrogen-bonding network may also form through the nitrogen atoms of the pyridine ring in this model.
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Fig. 3 Excitation and emission spectra of (a) LYH:Eu (λem = 613 nm, λex = 392 nm) and (b) NA-LYH:Eu (λem = 613 nm, λex = 268 nm). Inset: Photographs of LYH:Eu and NA-LYH:Eu under a 254 nm UV lamp. |
It is well known that UV energy absorbed by organic ‘antenna’ molecules can be transferred to the lowest excited state of RE3+ emitting centers through intersystem crossing from their S1 excited states to the lowest triplet (T1) states.42 This bypasses the forbidden transition rule and enhances the 4f–4f luminescence efficiency. Pure NA in an aqueous solution exhibits a strong absorption band centered at approximately 262 nm, attributed to the π → π* transition from the S0 ground state to the S1 excited state.43 Accordingly, the inclusion of NA in the LYH:Eu matrix was expected to sensitize the luminescence of Eu3+. Fig. 3b compares the PL spectra of LYH:Eu and NA-LYH:Eu. The excitation spectrum of NA-LYH:Eu, monitored at the 5D0 → 7F2 transition (613 nm), showed a strong broad band in the 220–300 nm range that was absent in the LYH:Eu host. This band, with significantly increased intensity, was attributed to the S0 → S1 (π, π*) transition of interlayer NA. The maximum intensity wavelength (approximately 268 nm) was close to the 262 nm π → π* transition of pristine NA, supporting this assignment. As shown in Fig. S2 (ESI†), the UV absorption band of NA remaining unchanged after the inclusion into the interlayer of LYH:Eu, coupled with the excitation at a similar wavelength, indicated minimal interaction between interlayer NA and the hydroxide layer. Upon excitation at 268 nm, the emission intensities related to the 5D0 → 7FJ transitions of Eu3+ increased significantly after NA inclusion (Fig. 3b). The bright red emission, predominantly from the 5D0 → 7F1 and 5D0 → 7F2 transitions near 600 nm, was distinctly visible under a standard 254 nm UV lamp (Fig. 3b, inset). This demonstrates that UV absorption by interlayer NA is followed by energy transfer to the 5D0 excited state of Eu3+, effectively sensitizing and enhancing Eu3+ luminescence in the NA-LYH:Eu layer via the “antenna” effect.
Interestingly, weak intra-4f6 transitions from the 7F0 ground state of Eu3+ were still observed in the 350–400 nm range, despite the dominance of the S0 → S1 transition of interlayer NA in the excitation spectrum of NA-LYH:Eu. This feature suggests that Eu3+ was excited not only through sensitization by NA but also directly via intra-4f6 transitions, highlighting a relatively low efficiency of energy transfer from the NA sensitizer to the Eu3+ emitting center. Effective energy transfer from a sensitizer to Eu3+ requires energy-level matching. The T1 state of NA (26385 cm−1) is higher than the 5D0 excited state of Eu3+ (17
250 cm−1),44,45 enabling energy transfer to occur. However, optimal energy transfer efficiency is achieved when the energy gap between the sensitizer's T1 state and the emitter's lowest excited state is within 2000–5000 cm−1, as larger gaps increase nonradiative transition pathways.46 The substantial energy difference (ΔE ∼ 9135 cm−1) between the T1 state of NA and the 5D0 state of Eu3+ likely contributes to the relatively inefficient energy transfer observed.
To investigate the exchangeability of interlayer NA with chloride ions, NA-LYH:Eu powder was reacted with a 0.5 M NaCl aqueous solution to simulate seawater conditions. As shown in Fig. 4, the XRD pattern of the sample after 24 h at RT revealed significant changes. The layered structure was preserved, as evidenced by the presence of (00l) reflections; however, the interlayer distance decreased from 14.7 Å to approximately 8.2 Å, consistent with the interlayer distance of LYH intercalated with chloride anions.25 TGA curves before and after the reaction (Fig. S3, ESI†) further supported this exchange. The weight loss attributed to the decomposition of interlayer NA at approximately 420 °C was nearly eliminated, while a new weight loss associated with the liberation of interlayer chloride appeared above 650 °C. The total observed weight loss (approximately 33.4%) was close to the calculated value (30.4%) for a Cl-LYH:Eu formulation containing only chloride anions. The slightly higher observed weight loss likely results from residual NA due to incomplete release. These results indicate that NA anions in LYH:Eu were replaced by chloride anions via a topotactic ion–exchange mechanism. The weak interaction between interlayer NA and the hydroxide layers of LYH:Eu, as suggested by the absence of significant shifts in the π → π* absorption wavelength of NA before and after inclusion (Fig. S2, ESI†) and the similarity in excitation wavelengths of free NA and NA-LYH:Eu (Fig. 3), likely facilitates this exchange. The high NA-loading capacity of LYH:Eu also implies a high chloride-uptake capacity, making it a potential candidate for chloride-trapping inhibitor. Additionally, the exchange process can be visually monitored in situ. As shown in the photographs in Fig. 4 insets, the red luminescence of colloidal solution containing NA-LYH:Eu powder under a 254 nm UV lamp was significantly diminished after reaction with chloride anions, allowing for clear visual differentiation. Fig. S4 (ESI†) compares the PL spectra of NA-LYH:Eu powder before and after reaction in the NaCl solution. The excitation spectrum monitored at λem = 613nm showed a substantial decrease in the intensity of bands attributed to energy transfer from interlayer NA, indicating the near-complete removal of interlayer NA. Upon excitation at 268 nm, the emission associated with the 5D0 → 7F2 main transition was also significantly reduced. This luminescence quenching, linked to NA release (or chloride trapping), was visually distinguishable under a commercial UV lamp.
The regeneration and recycling potential of LYH:Eu for repeated NA inclusion/release processes was also assessed. NA-LYH:Eu was reacted in the NaCl solution at RT to release interlayer NA, and the resulting powder was reused to uptake NA from an aqueous NA solution. This cycle was repeated 3 times, with the ‘luminescence-on/off’ behavior monitored under a 254 nm UV lamp. As shown in Fig. 5, the bright red emission of NA-LYH:Eu was restored after each regeneration, indicating successful reuptake of NA (‘luminescence-on’). Conversely, subsequent reaction in the NaCl solution quenched the red emission, reflecting NA release and chloride incorporation (‘luminescence-off’). Variations in the XRD patterns and TGA curves during repeated recycling processes are shown in Fig. S5 and S6 (ESI†). Despite the reduced crystallinity, the layered structure was preserved through three regeneration cycles. The relative weight loss gradually decreased with successive recycling, indicating that the regeneration of NA-LYH:Eu was not entirely effective. The NA loading capacity declined to approximately 85% after the third regeneration. Nevertheless, these results confirm that LYH:Eu retains its performance for NA inclusion and release, demonstrating its potential for multiple reuse cycles.
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Fig. 5 Photographs under a 254 nm UV lamp of LYH:Eu powder as a function of the ‘on/off’ behavior caused by the NA inclusion and chloride trapping, respectively. |
The rate of NA release can be controlled by adjusting the crystallinity and size of LYH:Eu particles. When the host was synthesized under moderate conditions (45 °C for 6 h, as opposed to 90 °C for 12 h), the intensity of (00l) reflections in the XRD pattern was significantly reduced (see Fig. S7b, ESI†), indicating the formation of particles with lower crystallinity. Fig. S8 (ESI†) presents FE-SEM images of NA-LYH:Eu particles synthesized using hosts prepared under two different conditions. Under milder conditions, crystal growth was suppressed, resulting in much smaller particle sizes. As shown in the inset of Fig. 6, NA release was accelerated by approximately 20% when LYH:Eu host synthesized at 45 °C for 6 h was used. Therefore, NA-LYH:Eu with varying crystallinity and particle size can be designed to control the release rate of NA in PBS.
To further investigate the release behavior of NA, the XRD patterns of solid residues collected at 1, 2, 3, and 5 days after adding NA-LYH:Eu powder to PBS were analyzed. As depicted in Fig. 7, no shift was observed in the position of (00l) reflections until after 5 days, suggesting that the interlayer distance was preserved during the release process. This result contrasts with the significant shift in (00l) reflections observed after just 1 day in a NaCl solution (Fig. 4). In PBS, where H2PO4− and HPO42− phosphorous oxyanions are prevalent, a change in interlayer distance is inevitable for the replacement of interlayer NA by these oxyanions in the interlayer space. Therefore, it is evident that the release of interlayer NA from NA-LYH:Eu in PBS did not occur via an anion–exchange reaction that would normally alter the interlayer distance. Instead, the diffraction intensity of the (00l) reflections decreased progressively, eventually showing an amorphous-like pattern after 5 days (see inset of Fig. 7). As proposed previously,48 the formation of an amorphous phase would result from the reaction of layer Y3+/Eu3+ ions with phosphorous oxyanions, forming insoluble yttrium/europium hydrogen phosphate hydrate complexes from the outermost layer of NA-LYH:Eu particles. Consequently, interlayer NA is released via the gradual collapse of the hydroxide layer structure, rather than through the conventional anion–exchange process. FE-SEM images of NA-LYH:Eu particles before and after the release reaction, shown in Fig. 8, further support this observation. The initially clean surface morphology of the plate-shaped particles was significantly degraded, forming a porous structure after the release reaction in PBS for 24 h. It is also important to note that the high affinity of RE ions for phosphate facilitates the formation of orthophosphates with extremely low water solubility, with pKsp values ranging from 24 to 26.49 Thus, Y3+/Eu3+ ions in the LYH:Eu layer network likely react with phosphorous oxyanions, promoting inner-sphere complexation at the surface.
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Fig. 8 FE-SEM images of NA-LYH:Eu particles (a) before and (b) after release reaction in PBS for 24 h (bar = 100 nm). |
Footnote |
† Electronic supplementary information (ESI) available: FT-IR and UV-vis spectra. Additional XRD patterns, TGA curves, PL spectra and FE-SEM images. See DOI: https://doi.org/10.1039/d4tc05448b |
This journal is © The Royal Society of Chemistry 2025 |