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Rationally designed In–CeO2/g-C3N4 S-scheme heterojunction photocatalyst with tuned redox ability for the photocatalytic degradation of pharmaceutical contaminants

Mazen R. Alrahilia, Mohamed Abdel Rafeab, Magdi E. A. Zakic, M. Khairyc, Mohamed R. El-Aassard, Sultan Albarakatie, Imran Shakirf, Abdullah K. Alanazig and Muhammad Aadil*h
aDepartment of Physics, College of Science, Taibah University, Madinah, Saudi Arabia
bDepartment of Physics, College of Science, Imam Mohammad Ibn Saud Islamic University (IMSIU), 11623 Riyadh, Saudi Arabia
cDepartment of Chemistry, College of Science, Imam Mohammad Ibn Saud Islamic University (IMSIU), Riyadh, 11623, Saudi Arabia
dDepartment of Chemistry, College of Science, Jouf University, PO Box 2014, Sakaka, Aljouf, Saudi Arabia
eDepartment of Physics, College of Science, University of Jeddah, Jeddah, Saudi Arabia
fDepartment of Physics, Faculty of Science, Islamic University of Madinah, Madinah 42351, Saudi Arabia
gDepartment of Chemistry, College of Science, Taif University, Taif, Saudi Arabia
hDepartment of Chemistry, Rahim Yar Khan Campus, The Islamia University of Bahawalpur, Rahim Yar Khan 64200, Pakistan. E-mail: Mhammad.aadil@iub.edu.pk

Received 16th September 2025 , Accepted 17th November 2025

First published on 1st December 2025


Abstract

Herein, the synthesis of an indium-doped cerium oxide/graphitic carbon nitride (In–CeO2/g-C3N4) S-scheme heterojunction aimed at optimizing photocatalytic degradation under visible light for the remediation of pharmaceutical wastewater is reported. The materials were synthesized via a hydrothermal process, in which pure CeO2 and In-modified CeO2 (In–CeO2) were initially synthesized, followed by the incorporation of g-C3N4 to produce the heterojunction. A series of characterization methods, such as X-ray diffraction (XRD), Fourier-transform infrared spectroscopy (FTIR), thermogravimetric analysis (TGA), and scanning electron microscopy (SEM), validated the effective synthesis and structural integrity of CeO2, In–CeO2, and In–CeO2/g-C3N4. The optical bandgap of the samples was determined, presenting a reduction from 2.97 eV for CeO2 to 2.69 eV for In–CeO2/g-C3N4, which facilitated better visible-light absorption. Photocurrent and electrochemical impedance spectroscopy (EIS) characterizations indicated enhanced charge separation and reduced recombination in the In–CeO2/g-C3N4 heterojunction. Photocatalytic experiments for the degradation of levofloxacin (LVX) demonstrated that the In–CeO2/g-C3N4 heterojunction achieved 85% degradation, significantly higher than those achieved by In–CeO2 (63%) and CeO2 (44%), highlighting the enhanced photocatalytic performance of the heterojunction. The higher photocatalytic activity is attributed to the formation of an S-scheme charge migration channel, enabling efficient charge separation. Results indicate that the In–CeO2/g-C3N4 heterojunction has great potential for water purification applications, particularly in degrading drug contaminants.


1. Introduction

Utilizing visible light for the photocatalytic degradation of organic pollutants is an economical and sustainable cleantech solution to the escalating environmental pollution and water contamination.1,2 Despite its promise, the development of photocatalysts is a challenging process because the conventional semiconductor materials, including TiO2,3,4 ZnO,5,6 and CeO2,7,8 have low quantum efficiency due to their electronic band structures (wide optical bandgaps), which prevent harnessing the visible part (∼43%) of solar light, and their photogenerated charge carriers (electron–hole pairs) recombine rapidly limiting their availability.9–11

Cerium oxide (CeO2), commonly known as ceria, is an emerging material in the realm of photocatalysts, which is resistant to photocorrosion and is chemically and thermally stable.12,13 The applicability of ceria as a promising photocatalyst is explicitly limited by its weak visible-light activity and high electron–hole pair recombination, which are crucial factors for visible-light-driven photocatalysis.14–16 Several investigations, including metal-doping, indicate that cerium oxide modification tunes the electronic structure and enhances the quantum efficiency.16–19 The rapid electron–hole recombination can be suppressed by coupling ceria with another photocatalytic material through the formation of heterostructure junctions, thereby increasing the availability of charge carriers for photocatalytic reactions.20–23

Assembling two different photocatalytic materials with distinct electronic properties to construct heterostructure junctions enhances charge separation, which is crucial for significant photocatalytic performance.24–26 These materials possess distinct electronic band structures that facilitate the migration and separation of photogenerated electron–hole pairs, enhancing the photocatalytic performance.27,28 For instance, S-scheme heterojunction formation involves the interfacial contact of two photocatalysts, in which band structure alignment results in the accumulation of holes in the valence band of one of the combining photocatalysts and electrons in the conduction band of the other photocatalyst, which is mainly compelled by the internal electric field.29 Graphitic carbon nitride g-C3N4 (g-CN), a polymeric compound with a layered structure of tri-s-triazine units, exhibits high thermal and chemical stability with excellent visible-light activity. The distinguished properties, which include non-toxicity, a unique metal-free framework, and a semiconductor with a medium band gap, enable its use as a sustainable catalyst for photodegradation applications. Despite these characteristics, g-CN exhibits low quantum efficiency due to a low absorptivity coefficient and sluggish electron–hole separation, which can be improved by modifying g-CN. Various reports present g-CN as a promising material for the fabrication of heterostructure junctions, as its unique structural framework favours interfacial contact.30,31 For instance, ZrO2/g-CN,32 Ce(MoO4)2/g-CN, g-CN/Bi2O2CO3–Bi4O7,33 Nd/Ni–LaFeO3/g-CN,34 CdMoO4/g-CN,35 ZnO/g-CN,36 Ni-MOF/g-CN,37 and ZnAl-LDH/g-CN38 include the g-CN-based material designs for wastewater decontamination applications. The findings reveal that these composite designs not only increase the optical response but also facilitate charge separation and transport primarily through the formation of heterojunctions.

Based on the facts described above, we synthesized a visible-light-activated In–CeO2/g-CN S-scheme heterojunction to facilitate charge separation and transport, thereby augmenting the effective photocatalytic removal of pharmaceutical pollutants. The hydrothermal method was used to synthesize pure CeO2 and its indium-modified form, In–CeO2, while melamine was calcinated for its thermal polymerization to prepare g-CN. Both the components, In–CeO2 and g-CN, were subjected to ultrasonication to fabricate the In–CeO2/g-CN heterojunction. The synthesized materials were characterized to investigate their crystal structure formation, thermal stability, microstructure, optical activity, and electrochemical response. The photocatalytic efficiency of In–CeO2/g-CN was estimated by degrading levofloxacin, a typical pollutant, showcasing the effect of heterojunction formation on photocatalytic performance. The present work aims to significantly contribute to the design of heterojunction materials for the photocatalytic degradation of pharmaceutical contaminants in wastewater remediation.

2. Experimental

2.1 Chemicals

The chemicals, including ceric ammonium nitrate (Sigma-Aldrich, (NH4)2[Ce(NO3)6], ≥ 98.5%), indium nitrate (Sigma-Aldrich, In(NO3)3, 99.99%), and melamine (Sigma-Aldrich, Powder, 99%), were used in the synthesis of CeO2, In–CeO2, and In–CeO2/g-CN materials. Levofloxacin (LVX, C18H20FN3O4), ethylenediaminetetraacetic disodium salt (Sigma-Aldrich, EDTA-2Na, 99%), silver nitrate (AgNO3), isopropyl alcohol (Sigma-Aldrich, IPA, 99%), and benzoquinone (Sigma-Aldrich, BZQ, 99%) were used in the photocatalytic activity investigation. All the standards were prepared in DI water (k < 6 µS cm−1).

2.2 CeO2 and In–CeO2 synthesis

The facile hydrothermal method was applied to synthesize pure CeO2 and In–CeO2 materials. Initially, 3 g of (NH4)2[Ce(NO3)6] was added to 70 mL of DI water while stirring until the formation of a clear solution, followed by the addition of 0.15 g In(NO3)3. The pH was raised to ∼10 with drop-by-drop addition of NH4OH, and the solution was poured into a Teflon cup enclosed in an autoclave (stainless steel-made), following the heating of the solution at 180 °C for 12 h. The precipitates collected were thoroughly washed with DI water multiple times to neutralize the pH and remove unreacted precursors, and then dried at 55 °C for 2 h.

2.3 Preparation of g-CN powder

The g-CN powder was prepared from melamine through thermal condensation.39 Experimentally, 2 g of the precursor powder was placed in a 25 cc (porcelain) crucible and heated at 550 °C for 6 h at 5 °C min−1. Upon the completion of the heating process, the crucible was removed from the furnace and allowed to cool naturally in the air. The pale, yellowish-colored g-CN formed was collected and stored in a dry environment.

2.4 In–CeO2/g-CN construction

The g-CN-based heterojunction of modified In–CeO2 was formed using an ultrasonication method. In the experiment, 0.9 g of In–CeO2 was poured into DI water (100 mL) and sonicated with an ultrasonic probe for 1 hour. Similarly, in a beaker (100 mL, DI water), 0.1 g of g-CN powder was separately sonicated. The resulting suspensions were mixed, followed by sonication again for 1 hour to enhance the interaction and dispersion of In–CeO2 with g-CN, assembling the In–CeO2/g-CN heterojunction (Fig. 1).
image file: d5ra07023f-f1.tif
Fig. 1 Schematic of the synthesis of CeO2 and In–CeO2 (hydrothermal), g-CN (calcination), and In–CeO2/g-CN (ultrasonication).

2.5 Characterization

The crystal structure formation and phase purity of the fabricated materials were investigated by powder XRD (X-ray Diffractometer, Shimadzu 6100 AS, Cu-Kα radiation, λ = 0.154 nm) and FTIR spectroscopy (Shimadzu IRAffinity-1S Spectrophotometer), while for thermal stability, TGA (Thermo Plus Evo, TG8120 Rigaku) was performed. The morphology was explored by SEM (Scanning electron microscope, FEI S50) and optical activity by UV-vis spectroscopy (Double-Beam Spectrophotometer, Jenway/6850). The electrochemical response was recorded on a three-electrode potentiostat (reference electrode = Ag/AgCl, working electrode = indium tin oxide-coated glass, and auxiliary electrode = Pt wire) in 1 M Na2SO4 electrolytic solution.

2.6 Photocatalytic (PC) efficiency

The PC efficiency of CeO2, In–CeO2, and In–CeO2/g-CN photocatalysts was evaluated by degrading LVX under a Xe lamp (300 W, UV cutoff filter λ > 420 nm) placed 20 cm above the reaction mixture. Initially, 0.05 g of CeO2, In–CeO2, and In–CeO2/g-CN were dispersed in LVX (10 mg L−1, 100 mL) solutions in three separate beakers. The resultant mixtures (LVX + photocatalyst) were kept in the dark and stirred for 40 minutes to acquire LVX adsorption–desorption equilibria on the catalyst surface. Afterward, the solutions were exposed to light to initiate LVX degradation, following the separation of samples from the working mixture to investigate the degradation process. The catalyst In–CeO2/g-CN was recovered by centrifugation and reused for LVX degradation under the same conditions. The percentage degradation (D) was calculated using the relation D(%) = (1 − Ct/C0) × 100,40 where Ct represents the LVX concentration at the specified time interval, while Co is its initial concentration.

3. Results and discussion

3.1 Structural features

The crystal structure formation and phase purity of the synthesized materials were verified via XRD patterns (2θ = 10°–80°), which are shown in Fig. 2(a). The peaks present at 2θ = 28.56°, 33.16°, 47.45°, 56.34°, 59.14°, 69.53°, 76.92°, and 79.12°, corresponding to the (111), (200), (220), (311), (222), (400), (331), and (420) diffraction planes, are consistent with the standard data (00-034-0394), confirming the formation of CeO2.41 The indium-modified material shows a variation in its diffraction peaks, which correspond to the structural changes caused by the different ionic sizes of dopant indium and the cerium host.42 Notably, the absence of any additional diffraction peaks for pure CeO2 and its indium-modified composition In–CeO2 confirms the phase purity and insertion of indium ions in the CeO2 lattice. The lower-intensity diffraction peaks in the XRD pattern of In–CeO2/g-CN correspond to the interaction between In–CeO2 and g-CN, causing microstructural changes.43,44 The distinct lattice vibrations of the synthesized materials were confirmed from the FTIR spectra, as displayed in Fig. 2(c). The presence of distinctive Ce–O and Ce–O–Ce vibrations at 460 cm−1 and 1052 cm−1 confirms the formation of the synthesized materials.45 The peaks at 1640 cm−1, 1426 cm−1, 1324 cm−1, and 1252 cm−1 in the spectra of g-CN and In–CeO2/g-CN can be attributed to C–N heterocyclic and aromatic stretching vibrations, while the peak at 810 cm−1 corresponds to the bending vibration (s-triazine units) of the g-CN framework.46–48 The additional –OH stretching and –OH bending observed indicate moisture adsorption on the material's surface.49,50 The thermal TGA plots showcasing the mass loss of the material against the applied temperature of CeO2, In–CeO2, and In–CeO2/g-CN are shown in Fig. 2(d). In the lower temperature zone (<300 °C), minute weight losses of 2.29% (CeO2), 3.03% (In–CeO2), and 3.60% (In–CeO2/g-CN) were observed, which are due to moisture removal. For the g-CN-based heterojunction material, in the higher temperature zone (400–600 °C), 7.93% of weight loss was witnessed, which corresponds to g-CN combustion.51
image file: d5ra07023f-f2.tif
Fig. 2 (a) XRD patterns, (b) enlarged view of the diffraction patterns (2θ = 26–32°), (c) FTIR spectra, and (d) TGA plots of the synthesized pure CeO2, modified In–CeO2, and the In–CeO2/g-CN heterojunction.

3.2 Morphological analysis

The microstructure and morphology of the synthesized CeO2, In–CeO2, and In–CeO2/g-CN materials were examined by SEM analysis, and the micrographs are presented in Fig. 3. For CeO2, a fine granular-type aggregation was observed, while for In–CeO2, the symmetry changes to irregular-sized crystallites with varying sizes. Indium modification not only changes the microstructure from granules to crystallites, but also from aggregation to dispersion of the material. The g-CN integration further increases dispersion, preventing agglomeration, as evident in Fig. 3(d), which is substantial for photocatalytic applications.
image file: d5ra07023f-f3.tif
Fig. 3 SEM images of (a) CeO2, (b) In–CeO2, and (c and d) In–CeO2/g-CN.

3.3 Optical properties

The optical properties of CeO2, In–CeO2, g-CN, and In–CeO2/g-CN materials were investigated by UV-vis absorption spectroscopy, and the absorption spectra observed for different materials are presented in Fig. 4(a). The synthesized materials feature absorption edges extending into the visible region. Notably, indium-modification and heterojunction formation with g-CN considerably enhances visible-light absorption, as evident from the red-shift in the absorption edge.52,53 Fig. 4(b) presents the Tauc plots generated to calculate the optical bandgap (Eg),54 and the materials CeO2, In–CeO2, g-CN, and In–CeO2/g-CN feature an Eg of 2.97 eV, 2.89 eV, 2.77 eV, and 2.69 eV, respectively. The In–CeO2/g-CN heterojunction (Eg = 2.69 eV) exhibits increased absorption, facilitating the separation of electron–hole pairs under visible light and rendering it promising for photocatalytic applications.
image file: d5ra07023f-f4.tif
Fig. 4 (a) UV-visible absorption spectra and (b) bandgap calculation from the Tauc plot model of the synthesized CeO2, In–CeO2, g-CN, and In–CeO2/g-CN.

3.4 Electrochemical response

The electrochemical responses of CeO2, In–CeO2, g-CN, and In–CeO2/g-CN materials were investigated to elucidate charge transfer kinetics and electron–hole recombination rates. The EIS results, presented as Nyquist plots in Fig. 5(a), reveal a distinct electrochemical response. The semicircle diameter in the Nyquist plot reflects the charge transfer resistance (Rct) at the working electrode–electrolyte interface.55 Notably, the In–CeO2/g-CN heterojunction exhibits a smaller semicircle diameter compared to its components, g-CN and In–CeO2, indicating lower Rct and faster charge transfer kinetics.56–58 The light-on photocurrent generation for the materials CeO2, In–CeO2, g-CN, and In–CeO2/g-CN is presented in Fig. 5(b). The significantly increased photocurrent density observed for In–CeO2/g-CN can be attributed to enhanced charge separation due to band structure alignment, which suppresses rapid electron–hole recombination.59,60 The heterojunction formation enhances charge transport, thereby increasing the availability of electron–hole pairs or their participation in the photocatalytic process.
image file: d5ra07023f-f5.tif
Fig. 5 (a) Nyquist plots and (b) photocurrent responses of the CeO2, In–CeO2, g-CN, and In–CeO2/g-CN materials.

3.5 PC activity

The PC activity of CeO2, In–CeO2, and In–CeO2/g-CN materials was estimated by degrading LVX. The UV-vis absorption data of the LVX samples separated from the aliquot at specified time intervals (in the presence of In–CeO2/g-CN) are presented in Fig. 6(a). The absorption intensity at λmax corresponds to the LVX concentration, which decreases, indicating LVX degradation. The absorption intensity rapidly declines in the presence of the photocatalyst In–CeO2/g-CN as compared to In–CeO2 and CeO2, which degrade LVX to a lower extent. In Fig. 6(b), the LVX degradation (%) over the synthesized catalysts is presented, which follows the order, CeO2 (44%) < In–CeO2 (63%) < In–CeO2/g-CN (85%). The order of photocatalytic efficiency is consistent with the optical properties and electrochemical responses of the photocatalysts, which feature facilitated electron–hole separation and transport in In–CeO2/g-CN, revealing its promising potential for photocatalytic applications.
image file: d5ra07023f-f6.tif
Fig. 6 (a) UV-vis absorption spectra of the samples collected during LVX degradation in the presence of In–CeO2/g-CN and (b) comparison of the catalytic efficiency.

The kinetics study of LVX degradation over the photocatalysts, CeO2, In–CeO2, and In–CeO2/g-CN, is shown in Fig. 7(a), which presents 1st-order kinetics for LVX degradation. The rate constants were calculated as 0.0075 min−1, 0.0123 min−1, and 0.0198 min−1, corresponding to CeO2, In–CeO2, and In–CeO2/g-CN. The scavenging study presented in Fig. 7(b) for LVX degradation in the presence of a photocatalyst with the highest photocatalytic efficacy, In–CeO2/g-CN, was performed using EDTA, AgNO3, IPA, and BQ for trapping holes (h+), electrons (e), hydroxyl radicals (HO˙), and superoxide radicals (˙O2), respectively. In the presence of AgNO3, the decline in LVX degradation was not significant, but in the presence of IPA, the degradation dropped considerably. The scavenging investigation presents the contribution of active species in the order e < h+ < ˙O2 < HO˙ for LVX degradation. A detailed comparison of the present work with previous findings is presented in Table 1.


image file: d5ra07023f-f7.tif
Fig. 7 (a) Kinetic studies of LVX degradation over CeO2, In–CeO2, and In–CeO2/g-CN, and (b) scavenging studies over In–CeO2/g-CN.
Table 1 Detailed comparison of the present work with previous studies
Sr. no. Photocatalyst Pollutant Conditions D(%) References
1 Ag-doped g-CN/Biochar Ciprofloxacin (CIP) 50 ppm CIP, 50 mg catalyst, visible-light, 4 h 70% 61
2 ZnO/g-CN Methyl orange (MO) 10 ppm MO, 50 mg catalyst, 400 W lamp 83.71% 62
3 Ni-doped α-Fe2O3/g-CN Ciprofloxacin (CIP) 10 mg per L CIP, 15 mg catalyst, solar light ∼660 Wm−2 82.1% 63
4 g-CN/Bi2O2CO3 Carbamazepine (CBZ) 20 ppm CBZ, 1 g of catalyst, sunlight, 180 minutes 98% 64
5 ZnCr2O4/g-CN Ciprofloxacin (CIP) 10 mg per L CIP, 75 mg of catalyst, Halogen lamp, 120 minutes 74.36% 65
6 Bi2MoO6/g-CN Ciprofloxacin (CFX) 10 mg per L CFX, 0.05 g of catalyst, LED light, 90 minutes 89.04% 66
7 In–CeO2/g-CN Levofloxacin (LVX) 10 mg per L LVX, 50 mg catalyst, Xe lamp (300 W, UV cutoff filter λ > 420 nm), and 80 minutes 85% Present study


Electronic band structure alignment and energy band energies hold vital significance in designing heterojunction materials with a specific scheme for charge migration. To get insights into the mechanism of LVX degradation over In–CeO2/g-CN, the energy band values, VB maxima (EVB) and CB minima (ECB) of g-CN and In–CeO2 were explored by applying the relations:67,68

ECB = χEe − 0.5 Eg

EVB = ECB + Eg
Here, “χ” is electronegativity, and Ee = 4.5 eV denotes the energy of a free electron on the hydrogen scale. The calculated energy band values were EVB = +2.42 eV for In–CeO2 and ECB = – 0.28 eV, while EVB = +1.43 eV and ECB = −1.34 eV for g-CN. Thermodynamically, pure In–CeO2 is unable to generate ˙O2 radicals due to ECB being higher than the required reduction potential (O2/˙O2 = −0.33 eV vs. NHE,69). Pure g-CN is unable to generate HO˙ radicals as it has an EVB value lower than the required oxidation potential (HO/HO˙ = 1.99 eV and H2O/HO˙ = 2.23 eV vs. NHE,70). But the scavenging studies reveal the generation of both ˙O2 and HO˙ radicals, which degrade LVX. As shown in (Fig. 8), the low-redox-potential carriers, e of In–CeO2 and h+ of g-CN, recombine, leaving behind the active e (g-CN) and h+ (In–CeO2),71,72 which participate in the reduction and oxidation reactions producing active radical species that degrade LVX.


image file: d5ra07023f-f8.tif
Fig. 8 (a) Schematic of the proposed S-scheme In–CeO2/g-CN heterojunction and (b) reusability and (c) before-and-after XRD pattern alignments to study the stability of the catalyst.

The reusability and structural stability of In–CeO2/g-CN were studied by LVX degradation in different runs, and the results are presented in Fig. 8(b and c). The photocatalyst retains ∼95% of its initial activity after multiple cycles, indicating good structural stability and recyclability; minor losses are likely due to insufficient catalyst recovery. The diffraction pattern of the recovered catalyst displays its structural stability, as no significant change was detected.

4. Conclusion

Pure CeO2 and its indium-modified composition, In–CeO2, were hydrothermally fabricated, while g-CN was synthesized through melamine calcination. The In–CeO2 material was dispersed on g-CN through ultrasonication to construct the S-scheme In–CeO2/g-CN heterojunction. XRD and FTIR analyses verified the formation of CeO2, In–CeO2, and In–CeO2/g-CN, with thermal stability indicated by TGA. SEM micrographs showcased the dispersion of In–CeO2, with g-CN preventing agglomeration. The In–CeO2/g-CN heterojunction increased visible-light absorption under λ > 420 nm illumination and facilitated charge separation via band structure alignment, forming an S-scheme of charge migration. The PC efficiency was evaluated by LVX degradation in the presence of catalysts, CeO2, In–CeO2, and In–CeO2/g-CN. The In–CeO2/g-CN catalyst exhibited a maximum LVX degradation of 85% (0.0198 min−1) compared to CeO2 and In–CeO2, which degraded LVX to an extent of 44% (0.0075 min−1) and 63% (0.0123 min−1), respectively. The formation of the In–CeO2/g-CN S-scheme heterojunction enables the recombination of low-redox-potential charge carriers (with low redox ability), preventing active charge carriers (high redox ability) from recombining and making them available for photocatalytic reactions. Despite the improved activity, the study is limited to a single pollutant and Xe-lamp illumination conditions; future work will evaluate performance under solar-simulated visible light and conduct advanced interfacial analyses such as XPS.

Author contributions

Mazen R. Alrahili (writing – original draft, validation), M. Abdel Rafea (funding acquisition, project administration, resources), Magdi E. A. Zaki (investigation, formal analysis), M. Khairy (data curation, validation), Mohamed. R. El-Aassar (investigation, data curation), Sultan Albarakati (software, methodology), Imran Shakir (visualization, formal analysis), Abdullah K. Alanazi (writing – review & editing), Muhammad Aadil (supervision).

Conflicts of interest

There are no conflicts to declare.

Data availability

Data will be available upon request.

Acknowledgements

This work was supported and funded by the Deanship of Scientific Research at Imam Mohammad Ibn Saud Islamic University (IMSIU) (grant number IMSIU-DDRSP2502).

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