Open Access Article
Mohamed Abdel Rafeaa,
Kashif Alib,
Mohamed I. Attiac,
M. M. Rasheda,
Mohamed R. El-Aassar
d,
Imran Shakire,
Abdullah K. Alanazif,
Sidra Mubeen*g and
Muhammad Aadil
*h
aDepartment of Physics, College of Science, Imam Mohammad Ibn Saud Islamic University (IMSIU), 11623, Riyadh, Saudi Arabia
bDivision of Science and Technology, Department of Zoology, University of Education, Lahore, Pakistan
cDepartment of Chemistry, College of Science, Imam Mohammad Ibn Saud Islamic University (IMSIU), 11623, Riyadh, Saudi Arabia
dChemistry Department, College of Science, Jouf University, Sakaka, 2014, Saudi Arabia
eDepartment of Physics, Faculty of Science, Islamic University of Madinah, Madinah 42351, Saudi Arabia
fDepartment of Chemistry, College of Science, Taif University, Taif, Saudi Arabia
gDepartment of Chemistry, The Women University, Multan, 60000, Pakistan. E-mail: Sidra.mubeen@wum.edu.pk
hDepartment of Chemistry, Rahim Yar Khan Campus, The Islamia University of Bahawalpur, Rahim Yar Khan 64200, Pakistan. E-mail: Muhammad.aadil@iub.edu.pk
First published on 24th March 2026
Photocatalysis offers a scalable route to safeguard water security by destroying persistent dyes and drug residues under sunlight. We report a dual-strategy enhancement of spinel chromium cobaltite (CrCo2O4, CCO) via nitrogen doping (NCCO) and carbon-nanotube (CNT) compositing (NCCO@CNTs), synthesized by wet-chemical precipitation (urea as N source) followed by ultrasonication with CNTs. XRD/FTIR confirm phase-pure spinel formation with N-induced lattice disorder; SEM/EDX show improved dispersion and homogeneous N/Cr/Co/O/C distribution; UV-Vis/Tauc reveal band-gap narrowing from ∼3.0 eV (CCO) to ∼2.65 eV (NCCO); transient photocurrent demonstrates possible effective charge separation in NCCO@CNTs. Under natural sunlight (7 ppm, 25 mg catalyst, 75 mL), NCCO@CNTs degrades methylene blue (MB) and amoxicillin (AMX) by 90.7% and 85% in 60 min, surpassing NCCO (65.7%, 62%) and CCO (49.5%, 47.5%). Pseudo-first-order kinetics yield rate constants k(MB) = 0.037, 0.017, 0.011 min−1 and k(AMX) = 0.030, 0.015, 0.010 min−1 for NCCO@CNTs, NCCO, and CCO, respectively (≥3× over pristine CCO). Radical-trapping pinpoints ˙O2− and ˙OH as dominant species, aligning with a mechanism wherein N-doping broadens visible-light absorption/creates shallow states, while CNTs act as rapid electron sinks, suppressing e−/h+ recombination and adding adsorption/active sites. Benchmarking against reported spinel's indicates competitive or superior sunlight activity. By optimizing the performance of CrCo2O4 through dual modification (nitrogen doping and CNT compositing), this work enhances its photocatalytic activity, enabling effective degradation of a wide range of chemically distinct pollutants, and offers a scalable solution for practical wastewater remediation.
Organic dyes like methylene blue and Rh–B dyes are widely used in the textile, paper, and cosmetic industries, as well as in the pharmaceutical industry. Although intended and valuable for their desired purposes, these dyes are well known for their photochemical and biodegradation stability. When discharged into water bodies, they are long-lasting, bringing adverse effects to waterborne organisms.5 For instance, methylene blue may reduce light penetration in aquatic plants and consequently lead to low oxygen levels to the extent that plant and animal structures in the water adjust and finally die off. Environmental degradation has become an inevitable consequence of the fast economic and technological progress in recent decades. Antibiotics like levofloxacin, ciprofloxacin, amoxicillin, and tetracycline have become major environmental pollutants because of their usage in human and veterinary medicine.6–8 These antibiotics are anticipated to provide sufficient and potent inhibition against bacteria, hence their usage in treating bacterial infections. However, due to misuse and inadequate discharging of these antibiotics, they have been found to precipitate in various compartments in the environment, such as rivers, lakes, and groundwater.9,10
Photocatalysis has become a substantial technique for the catalytic decomposition of organic pollutants, including drugs, dyes, pesticides, etc. The efficiency of the photocatalytic processes mainly depends on the performance of the photocatalyst, but challenges persist in achieving stable light-to-electron conversion.11 Semiconductor materials are widely utilized for the degradation of antibiotic contaminants and organic dyes in wastewater due to their cost-efficiency, stable nature, tunable band gaps, variable oxidation states, and extended absorption spectra, enabling efficient photocatalytic activity. TiO2, SnO2, PbO2 and ZnO are frequently employed in photocatalytic applications.12 Despite the widespread utilization of these photocatalysts, their photocatalytic activity diminishes over time due to certain recurrent flaws. The key flaws are the poor separation of charge carriers, rapid recombination of charge carriers, too large band gap, and the need for UV light to excite electrons. All of these aspects add up to reducing their overall efficiency, constraining their practical applications, and rendering them less appropriate for sustainable environment purification.13
The AB2O4 spinel framework—hosting a divalent A cation and trivalent B cation—supports broad functionality in photocatalysis, energy devices, and sensing due to its adaptable structure.14,15
The cobalt chromite, CrCo2O4, a prominent member of the spinel structured semiconductive material used extensively in catalytic applications. Using controlled, position-specific partial doping—swapping Cr2+ and Co3+ at octahedral and tetrahedral sites with suitable metal or non-metal dopants—one can systematically tailor electronic and optical responses, thereby upgrading the material's photocatalytic efficacy.16 However, native CrCo2O4 tends to show limited visible-light absorption, insufficient charge separation, and fast recombination. Remedies include nitrogen doping and composite design; N-doping narrows the band gap and introduces controlled defects that help separate carriers.17
Carbon nanotubes (CNTs), when reinforced with the semiconductive photocatalytic materials, act as co-catalysts and strengthen the photocatalyst in three complementary ways:18,19 Firstly, being extremely conductive, it raises electrical conductivity of the resultant composite, hence promoting charge transport. Secondly, owing to its larger specific surface area and one-dimensional structure feature, it gets entangled with semiconductive material particles and suppresses their agglomeration, which results in it furnishing abundant active sites to adsorb pollutants, boosting degradation rates. Thirdly, being a carbonaceous material, it exhibits a broad optical absorption range; hence, on reinforcing with semiconductive material, it can improve solar light harvesting and overall activity.20,21 Synergism is realized by introducing nitrogen doping and CNT composite development, which addresses the shortcomings of CrCo2O4 and substantially enhances its photocatalytic performance for environmental cleaning.
Here in the current study, we have prepared chromium cobaltite (CrCo2O4, CCO) and nitrogen-doped chromium cobaltite (N-CrCo2O4, NCCO) through wet chemical method. The N-CrCo2O4@CNTs composite was prepared using an ultrasonication approach, which allowed suitable distribution of carbon nanotubes (CNTs) into the nitrogen doped spinel structure. The prepared materials were characterized in detail to confirm the integrity of their structure, morphology and composition using XRD, SEM, EDX and FTIR. The optical and opto-electronic properties of the materials were also studied to examine their feasibility for photocatalytic applications. The synergistic effects of N-doping and CNT composite formation were investigated for the photocatalytic activity of the prepared NCCO@CNTs by degrading two different pollutants in water, one arising from textile (methylene blue dye) and another from pharmaceutical industries (amoxicillin). These pollutants were chosen to mimic complex, multi-pollutant polluted water, indicating that the resulting products have potential applications for wider treatment of contaminated water.
| S. no. | Name | Formula | Purity | Supplier |
|---|---|---|---|---|
| 1 | Cobalt nitrate hexahydrate | Co(NO3)2·6H2O | 99% | Sigma-Aldrich |
| 2 | Chromium nitrate | Cr(NO3)3·9H2O | 99% | Sigma-Aldrich |
| 3 | Deionized water | H2O | — | Sigma-Aldrich |
| 4 | Urea | CO(NH2)2 | 99% | Sigma-Aldrich |
| 5 | Sodium hydroxide | NaOH | 98% | Sigma-Aldrich |
| 6 | Carbon nanotubes (dispersed) | CNTs | 5–10 mg L−1 | Sigma-Aldrich |
:
1 molar ratio was dissolved in 150 mL of deionized water. To adjust the pH to 11, a 2.0 M NaOH solution (50 mL) was added dropwise. The mixture was agitated for 30 min until a dark green colour developed and precipitates formed. The reaction mixture was then washed well several times with double-distilled water after precipitation to neutralize and eliminate excessive by-products of reactants. The precipitate was collected and dried in an oven at 100 °C for 12 h and annealed at 400 °C for another 4 h in furnace to crystallize. The CCO product obtained was observed as dark green powder.
The synthesis of nitrogen-doped chromium cobaltite was realized in a similar manner to CCO, with urea added to the solution at the beginning of the procedure, as given in Fig. 1 (step-I). Urea served as a source of nitrogen to enter its atoms into the spinel frame and thereby change its properties, making it more suitable to be a photocatalyst. The composite sample containing NCCO and CNTs was then prepared by adopting well know ultrasonication methodology. The weight % of the NCCO and CNTs were kept 85% and 15% respectively. The NCCO and CNTs were dispersed in water and sonicated the suspension of 1 hour at 80 °C, as shown in Fig. 1 (step-II). Then, the water was slowly evaporated by keeping the predeparture below the boiling point of water and solid composite sample was achieved.
![]() | (1) |
![]() | (2) |
This method allows for a comprehensive evaluation of the photocatalytic performance of NCCO and NCCO@CNTs for degrading different concentrations of organic pollutants, contributing to their evaluation for environmental applications.
The sharpness of the diffraction peaks ensures the satisfactory crystallinity, while the nonexistence of any irrelevant peak ensures the purity of the prepared CCO. In NCCO, even after N-doping, no additional diffraction peaks were detected. Nevertheless, one can observe three prominent differences in the diffraction pattern that occurs following N-doping. First, a decrease in peak intensity was noticed. This weakened intensity may result from the lattice defects and disorder introduced by N doping. These defects disrupt the regular atomic arrangement, scattering X-rays and lowering the diffraction signal. Second, a small shift towards the higher 2θ values was found meaning that lattices have shrunk owing to smaller nitrogen atoms than larger ones being replaced and d-spacing were reduced which lead diffraction peaks shifting to higher angles. Third, a broadening of the peaks was also found in NCCO XRD pattern indicating some structural disorder due to the introduction of nitrogen. The broadening of FWHM can be attributed to smaller crystallite sizes, which is caused by lattice defects and quantum confinement effect upon the introduction of nitrogen. The domain/crystallite size was estimated by the Scherrer relation (eqn (3)).25
![]() | (3) |
The average domain/crystallite size of CCO was 20.16 nm and that of NCCO was 16.19 nm, which again supported the findings of maximum peak broadening in case of NCCO. The NCCO@CNTs nanocomposites had an additional weak hump around 24–25° 2θ, which was caused by CNTs (absent in the XRD patterns of CCO or NCCO as individual materials). This peak and the presence of diffraction peaks for both NCCO and CNTs indicates that the synthesis of the NCCO@CNTs nanocomposite has been successful.
The typical FTIR spectra of the CCO, NCCO, and NCCO@CNTs, recorded using a Thermo Fisher Nicolet IS5, are shown in Fig. 2b, revealing a number of characteristic bands that can be used for the analysis of structural and bonding features in these materials. The transmittance bands of metal–oxygen (M–O) stretching vibrations occurring at octahedral and tetrahedral sites are identified in the CCO sample at 446 cm−1 and 613 cm−1, respectively. These bands confirm the formation of a spinel-phase structure for CCO. The relatively weaker intensity of the band at 446 cm−1 compared to the 613 cm−1 band can be explained by the longer and weaker M–O bonds at the octahedral sites.26 For the NCCO sample, these two bands redshift slightly. This trend suggests that the existence of structural defects or distortion from the doping nitrogen weakens the M–O bond.27 NCCO@CNTs sample shows a full set of bands of NCCO and an extra weak band at 1500 cm−1 assigned to the C
C stretching vibration mode of the nanotubes (CNTs). The low intensity observed for this band can be explained by the non-polar character of the C
C bonds, thus negligible dipole moment alteration takes place during vibration.28,29 Also, in case of all samples, a band at 1604 and 3445 cm−1 are observed that are attributed to the bending and stretching vibration of O–H groups, respectively.30,31 These bands are assigned to the absorbed moisture of the samples. Moreover, one signal appearing at around 2346 cm−1 in all the samples is assigned to the asymmetric stretching vibration of O
C
O group related to absorbed CO2.32
000 indicate that the shape of particles is mostly aspherical and most of them are smaller than 100 nm in diameter.
However, larger micro-sized aggregates are also present on the CCO particles. Such bulky structures indicate an extent of agglomeration and may interfere with the dispersion of the material. The formation of bulky structures reduces the exposed surface area, consequently impeding the photocatalytic activity of the CCO material. These findings indicate that the agglomeration of the CCO particles limits their performance in photocatalytic applications, where surface interaction and the availability of active sites are critical. By contrast, the SEM image of the NCCO@CNTs using a higher magnification (×40
000), as shown in Fig. 3b, indicates that the particles are more spherical in shape and have better dispersions than those of the CCO sample.
The presence of CNTs in the matrix of NCCO is responsible for inhibiting the formation of large clusters. While a few minor clusters evidenced by the dashed circles are still visible, their size is considerably smaller than the domination clusters of the CCO sample. The NCCO particles interact well with the CNTs to enable the inhibition of particle agglomeration and maintain good particle dispersion. This uniform dispersion enhances the available surface area and improves the material's photocatalytic performance. The NCCO particles have mostly filled the unevenly sized and shaped voids that were created by the random entanglement of the CNT particles. This not only makes the particles interact better, but it also stops them from sticking together on their own.
Energy-Dispersive X-ray Spectroscopy (EDX) analysis was conducted to verify the chemical structure and purity of the synthesized NCCO@CNTs composite. The EDS spectrum shown in Fig. 4a clearly identifies the presence of key elements: nitrogen (N), chromium (Cr), cobalt (Co), oxygen (O), and carbon (C), with a prominent C peak corresponding to the carbon nanotube (CNT) matrix integrated into the composite. The absence of any undesirable peaks further confirms the successful synthesis of the NCCO@CNTs composite and the chemical homogeneity of the hybrid material.
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| Fig. 4 (a) EDX spectrum of NCCO@CNTs, and (b–g) elemental mapping images confirming uniform distribution of N, Cr, Co, O and C. | ||
Fig. 4b–g are the elemental distribution maps of N, Cr, Co, O, and C showing a homogeneous and well-distributed incorporation of these elements into the composite structure. The distribution of these elements is important in ensuring the optimal transfer of charge and surface reactivity, which are major determinants of the increased photocatalytic activity of the material.33 The addition of CNTs allows for better dispersion of the NCCO nanoparticles and allows for interactive interaction between the two materials, hence optimizing the photocatalytic activity for environmental purpose.
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| Fig. 5 (a) Optical absorption characteristics and (b) transient photocurrent response of CCO, NCCO, and NCCO@CNTs. | ||
On the other hand, the NCCO sample exhibits a redshift of the absorption edge to the visible region, which is contributed by the bandgap reduction arising from nitrogen doping. The absorption range of the composite is also broadened into visible wavelengths. CNTs instead improve the light absorption availability to the structure by increasing the material's spectral coverage and augmenting its light harvesting properties, especially in the visible region, originating from its black body nature.32 By following the below given relation (eqn (4)),34 the bandgap of CCO was 3.0 eV, whereas nitrogen doping reduced the bandgap of NCCO to 2.65 eV.
| (αhv)1/2 = A(hv − Eg) | (4) |
This reduction facilitates better absorption of visible light, improving NCCO's photocatalytic performance by utilizing a wider range of the solar spectrum.35 These results emphasize that nitrogen doping and CNT integration are effective approaches to enhance the light absorption and photocatalytic efficiency of CrCo2O4, making it suitable for environmental applications.
To examine the role of nitrogen doping and CNT incorporation in modulating possible charge separation, transient photocurrent profiles of CCO, NCCO, and NCCO@CNTs were recorded (Fig. 5b). The lowest photocurrent density was recorded for CCO. In contrast, N-doping resulted in a significant increase attributed to bandgap narrowing and the formation of shallow donor states, which improved the likelihood of photoexcitation. However, recombination within the spinel lattice continued to restrict carrier utilization.33,36 A higher efficiency was obtained in the presence of CNTs, whose conductive network functioned as an active electron sink for promoting photoinduced NCCO to be extracted as soon as it is photoexcited and avoiding recombination, allowing an effective charge transport over longer distances toward the collector. The collaborative utilization of NCCO@CNTs leads to a higher photocurrent density compared to pristine CCO and NCCO.
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| Fig. 6 Time-dependent UV-Vis spectra showing MB dye degradation over (a) CCO, (b) NCCO, and (c) NCCO@CNTs, (d) with corresponding degradation percentages and (e and f) kinetic analysis. | ||
The further enhancement in the MB dye degradation efficiency, that is from 65.7% (NCCO) to 90.7% (NCCO@CNTs), could be attributed to the incorporation of CNTs. Where CNTs greatly facilitate the charge collection, acting as the conductive networks and for suppressing recombination of electron–hole and providing a large surface area for adsorption of pollutants.37,38 Both nitrogen doping and CNT introduction in NCCO@CNTs contribute to the best photocatalytic property and illustrate the synergy of these two modifications.
Based on the results of kinetic models applied to the degradation data, the selected kinetic model was pseudo-first-order kinetic, based on an R2 value close to unity. The degradation of MB dye follows a pseudo-first-order kinetic pattern as seen in Fig. 6e and f, where NCCO@CNTs decay rate is the fastest. The rate constant (k) for CCO was 0.011 min−1, increasing to 0.017 min−1 for NCCO and 0.037 min−1 for NCCO@CNTs, demonstrating a 3.36-fold enhancement over CCO. The enhanced efficiency can be explained by the synergistic effect of N doping and CNT reinforcement, which results in accelerated charge transfer, improved light harvesting ability, and an increase in surface reactive sites. In conclusion, a nitrogen-doped and CNT-loaded composite strongly enhances photocatalytic activity, leading to faster disappearance of MB dye in the presence of solar light.39
The photocatalytic degradation of amoxicillin over CCO, NCCO, and NCCO@CNTs was monitored by UV-Vis spectroscopy (Fig. 7a–c). The characteristic absorption band of amoxicillin at 230 nm gradually diminished with irradiation time, confirming its breakdown under solar light. After 60 min, the extent of removal followed the order NCCO@CNTs (85%) > NCCO (62%) > CCO (47.5%), as summarized in Fig. 7d.
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| Fig. 7 Time-dependent UV-Vis spectra showing AMX degradation over (a) CCO, (b) NCCO, and (c) NCCO@CNTs, (d) with corresponding degradation percentages and (e and f) kinetic analysis. | ||
Similar to the MB dye case, amoxicillin degradation improved step by step. Nitrogen doping upgrades the catalyst by narrowing the bandgap and stabilizing charge carriers. CNTs further enhance activity by making charge transport easier, reducing recombination, and expanding the reactive surface.40
The kinetic study (Fig. 7e and f) shows that amoxicillin degradation follows a pseudo-first-order reaction with an acceptable fit (R2 = 0.99). The rate constant increased from 0.010 min−1 for CCO to 0.015 min−1 for NCCO and 0.030 min−1 for NCCO@CNTs, giving the composite nearly three times the activity of CCO due to faster charge transfer and less recombination.
Our results agree on one point: the modifications work, as both the faster kinetics and higher efficiencies point to the same conclusion-nitrogen doping improves light harvesting, and CNTs prevent recombination, together building a better photocatalyst. Table 2 highlights this with side-by-side data for MB dye and amoxicillin, proving the strategy works for both dyes and pharmaceutical residues.
| S. no. | Photocatalyst | Pollutant | Light source | % Degradation | Rate constant (min−1) |
|---|---|---|---|---|---|
| 1 | CCO | Methylene blue | Sunlight | 49.5 | 0.011 |
| 2 | NCCO | Methylene blue | Sunlight | 65.7 | 0.017 |
| 3 | NCCO@CNTs | Methylene blue | Sunlight | 90.7 | 0.037 |
| 4 | CCO | Amoxicillin | Sunlight | 47.5 | 0.010 |
| 5 | NCCO | Amoxicillin | Sunlight | 62 | 0.015 |
| 6 | NCCO@CNTs | Amoxicillin | Sunlight | 85 | 0.030 |
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| Fig. 8 Effect of different radical scavengers on the photocatalytic degradation of (a) MB dye and (b) amoxicillin over NCCO@CNTs, and (c and d) compare the corresponding degradation efficiencies. | ||
The MB dye removal efficiency (Fig. 8a and c) dropped from 90.7% to 83% (AgNO3), 71% (EDTA), 56% (2-propanol), and 44% (P-BQ). This pattern shows superoxide radicals are the most decisive factor, hydroxyl radicals and holes have a strong effect too, and electrons are the least involved. As seen in Fig. 8b and d, amoxicillin degradation followed the same order of scavenger effects: 81% (AgNO3), 68% (EDTA), 49% (2-propanol), and only 43% (P-BQ).
The major influence of P-BQ and 2-propanol highlights that superoxide and hydroxyl radicals are the key species, while the rest contribute less. Since P-BQ and 2-propanol caused the biggest drop-in activity, we know superoxide and hydroxyl radicals are the central species in this reaction. For a fair comparison, Table 3 presents our results alongside those of other spinel oxide photocatalysts, highlighting the relative performance of our material.
| S. no. | Photocatalysts | Pollutant | Light source | Degradation (%) | References |
|---|---|---|---|---|---|
| 1 | ZnCo2O4 | Methylene blue | Sunlight | 41.97 | 42 |
| 2 | Ag–ZnCo2O4 | Methylene blue | Sunlight | 58.02 | 42 |
| 3 | ZnCo2O4 | Crystal violet | Tungsten bulb | 61.6 | 43 |
| 4 | CuO/ZnCo2O4 | Crystal violet | Tungsten bulb | 78 | 43 |
| 5 | CuO/ZnCo2O4/CNTs | Crystal violet | Tungsten bulb | 87.7 | 43 |
| 6 | NiCo2O4 | Methyl red | Visible light | 95.1 | 44 |
| 7 | NiCo2O4/gC3N4 | Congo red | Solar light | 65 | 45 |
| 8 | NiCo2O4/gC3N4 | Rhodamine B | Solar light | 50 | 45 |
| 9 | N–CrCo2O4@CNTs | Methylene blue | Sunlight | 90.7 | Current work |
| 10 | N–CrCo2O4@CNTs | Amoxicillin | Sunlight | 85 | Current work |
| EVB = χ − Ee + 0.5Eg | (5) |
| ECB = EVB − Eg | (6) |
![]() | ||
| Fig. 9 Schematic of the charge-transfer and reactive species pathways in the photocatalytic degradation of pollutants by NCCO@CNTs. | ||
The mechanism of the composite-driven degradation is proposed as visible-light excites NCCO via photons with energy matching or exceeding its bandgap. This process moves electrons up into the conduction band, leaving holes in the valence band. The EVB is sufficiently positive (2.775 vs. NHE) to facilitate the oxidation of both water and hydroxide ions into highly reactive hydroxyl free radicals. Hydroxyl free radicals, being several times more reactive than simple holes, attack the pollutant molecules and degrade them. The conduction band (CB) potential by itself is not sufficiently negative (0.125 vs. NHE) to reduce oxygen directly into superoxide radicals (˙O2−).46,47
CNTs play a helpful role at this point through immediate acceptance of the excited electrons, eliminating the chances of their recombination and stabilizing them long enough to transfer to O2 molecules. This transfer of electrons to oxygen forms ˙O2−. The hydroxyl and superoxide radicals have a synergistic effect to degrade pollutants. VB hole oxidizes water or hydroxide for ˙OH formation. CNTs stabilize and donate an electron to oxygen for ˙O2− creation. The two radicals work together to quickly and efficiently degrade the pollutant molecules-degrading drugs and dyes-into harmless mineralized forms.
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