2. Results and Discussion
Field-emission scanning electron microscopy (FESEM) was employed to characterize the surface morphology of the synthesized materials. The as-prepared g-C
3N
4 (g-CN) exhibited a typical 2D lamellar sheet-like structure (
Figure 1a), providing a suitable platform for the subsequent integration of semiconductor nanoparticles. Energy-dispersive X-ray (EDX) spectroscopy confirmed the composition of g-CN, with a C/N atomic ratio of 0.82, approximating the theoretical value of 0.75 (
Figure 1a’). Sulfonic acid functionalization did not alter the fundamental 2D morphology of g-CN (SA-g-CN) (
Figure 1b). The successful introduction of -SO
3H groups was verified by EDX analysis (
Figure 1b’). BiOI exhibited a distinctive thin nanoplate structure (
Figure 1c), as revealed by FESEM. The corresponding elemental composition is presented in
Figure 1c’. The g-CN/BiOI composite displayed a homogeneous distribution of BiOI nanoparticles on the g-C
3N
4 surface (
Figure 1d). EDX analysis confirmed the presence of all constituent elements (
Figure 1d’). The SA-g-CN/BiOI nanocomposite maintained the morphological characteristics of g-CN/BiOI (
Figure 1e), emphasizing the role of the 2D lamellar structure of SA-g-CN. EDX analysis of SA-g-CN/BiOI (
Figure 1e’) corroborated the presence of all expected elements. Additionally, elemental mapping analysis of SA-g-CN/BiOI (
Figure 1f) visually confirms the successful sulfonic acid functionalization, the uniform distribution of BiOI on the g-C
3N
4 surface, and the formation of a heterojunction composite.
X-ray diffraction (XRD) (
Figure 2a) analysis revealed characteristic peaks at approximately 13.0° and 27.6° in both pristine g-CN and SA-g-CN, corresponding to the (100) and (002) crystal planes, respectively. These peaks are attributed to the in-plane structural packing and interlayer stacking of the graphitic g-CN structure (JCPDS No. 87-1526) [
27]. While CN-SAF exhibited a similar diffraction pattern, a reduction in the intensity of the 27.6° peak was observed, indicating an increased interlayer spacing due to the incorporation of surface-functionalized sulfonic groups. XRD patterns of pure BiOI exhibited characteristic peaks at 9.65°, 29.6°, 31.6°, 37.0°, 39.3°, 45.9°, 51.3°, 55.1°, 60.2°, and 61.5°, corresponding to the (001), (102), (110), (103), (004), (200), (114), (212), (115), and (204) planes, respectively. These diffraction patterns confirmed the formation of a tetragonal phase (space group
P4/nmm) for the BiOI nanoplates (JCPDS No. 96-434-1501) [
28]. The XRD patterns of both g-CN/BiOI and SA-g-CN/BiOI composites displayed characteristic peaks corresponding to both SA-g-CN (marked as spades) and BiOI (marked as diamonds), providing evidence for the successful formation of heterojunction structures.
Fourier transform infrared spectroscopy (FTIR) investigation (
Figure 2b) was employed to identify the functional groups and chemical bonds present in the synthesized nanomaterials. The FTIR spectra of pristine g-CN and SA-g-CN, recorded in the 400–4000 cm
−1 region, exhibited characteristic vibrational bands. Pure g-CN displayed characteristic absorption bands between 1200 and 1600 cm
−1, attributed to the C–N heterocycles within the heptazine units. A sharp peak at 807 cm
−1 corresponded to the stretching vibrations of C–N–C moieties in the triazine ring [
29]. In contrast, the spectrum of SA-g-CN revealed additional peaks at 615 and 796 cm
−1, assigned to the bending vibrations of –SO and C–N–S groups, respectively, indicating the successful incorporation of sulfonic acid functional groups. Furthermore, the presence of surface sulfonic groups was confirmed by vibrational bands at 968 and 1124 cm
−1. A broad absorption band observed between 3060 cm
−1 and 3300 cm
−1 was attributed to the stretching vibrations of –NH, =NH, and –OH groups originating from uncreated amino groups and adsorbed water [
30]. On the other hand, the FTIR analysis revealed a characteristic peak at 571.5 cm
−1 attributed to the symmetric stretching vibration of the Bi-O bond in BiOI. Additionally, strong absorption bands were observed within the 1300–1700 cm
−1 region, likely associated with the presence of organic impurities or adsorbed species. A broad and intense peak centered around 3350 cm
−1 indicated the presence of adsorbed water molecules, with contributions from both bending (∼1650 cm
−1) and stretching (∼3500–3000 cm
−1) vibrational modes of hydroxyl groups (–OH) [
31]. Correspondingly, the FTIR spectra of g-CN/BiOI and SA-g-CN/BiOI exhibit the combined vibrational bands of SA-g-CN and BiOI, which confirms the excellent formation of heterojunction composite.
X-ray photoelectron spectroscopy (XPS) was employed to investigate the chemical environment and bonding interactions within the catalytic nanocomposites.
Figure 3a presents survey spectra (0 to 1000 eV) of SA-g-CN, BiOI, and SA-g-CN/BiOI, confirming the presence of the expected elements. High-resolution spectra of C 1s, N 1s, Bi 4f, O 1s, and I 3d are shown in
Figure 3b–f. Deconvolution of the C 1s spectra from pristine SA-g-CN and SA-g-CN/BiOI revealed two peaks at 284.76 and 287.9 eV, attributed to C–C and N–C=N bonds, respectively. Similarly, the N 1s spectra exhibited peaks at 398.52 and 400.21 eV, corresponding to pyridinic and graphitic nitrogen. Compared to the pristine SA-g-CN, the C 1s and N 1s peaks in SA-g-CN/BiOI shifted to higher binding energies. This suggests an increase in electron density/cloud or a change in the electronic structure of SA-g-CN upon contact with BiOI under light irradiation, possibly due to interfacial charge transfer. Further XPS analysis of the S 2p region (
Figure S1) revealed two distinct peaks at 164.79 and 168.11 eV, indicative of –SH and –SO
3H groups, respectively, confirming the successful sulfonic acid functionalization of g-CN. Due to spectral overlap with bismuth, the S 2p spectrum of SA-g-CN/BiOI could not be clearly distinguished. The Bi 4f spectrum exhibited two prominent peaks at 158.13 and 163.54 eV, corresponding to the Bi
3+ states of Bi 4f7/2 and Bi 4f5/2. The O 1s spectrum of SA-g-CN was deconvoluted into two peaks at 531.55 and 533.46 eV, attributed to the –SO
3H and –OH groups of the sulfonic acid functional groups. In SA-g-CN/BiOI, the O 1s spectrum showed peaks at 529.94 and 532.06 eV, corresponding to Bi–O and surface-bound hydroxyl (–OH) groups, respectively. The I 3d spectrum of BiOI displayed two significant peaks at 619.08 and 630.57 eV, attributed to I 3d5/2 and I 3d3/2. The observed higher binding energy shifts for Bi 4f and I 3d in the SA-g-CN/BiOI heterojunction catalyst suggest an increased electron density, likely due to enhanced photogenerated charge transfer across the heterojunction interface.
The optical absorption properties of the prepared samples were investigated using UV-Vis diffuse reflectance spectroscopy (UV-DRS) (
Figure 4a). Both pristine g-CN and SA-g-CN exhibited absorption edges at approximately 469.8 nm, indicating a primary response to the UV region of the spectrum. In contrast, BiOI demonstrated enhanced visible light absorption with a band edge centered at approximately 690 nm. Interestingly, the g-CN/BiOI and SA-g-CN/BiOI composites displayed red-shifted absorption edges, reaching approximately 685 nm and 715 nm, respectively. These results suggest that the incorporation of BiOI significantly improved visible light absorption and potentially reduced bandgap energies, which are essential parameters for efficient photo(electro)catalytic processes.
The bandgap energy (E
g) was estimated through Tauc plots (
Figure 4b) constructed using the Kubelka–Munk function (Equation (1)) [
32]. This equation relates the absorption coefficient (α) to the photon energy (hν):
where A is a proportionality constant, h = Planck’s constant, Eg = bandgap energy, and n is a transition coefficient with values of 1/2 for direct allowed transitions and 2 for indirect allowed transitions. The calculated bandgap energies (E
g) for g-CN, SA-g-CN, BiOI, g-CN/BiOI, and SA-g-CN/BiOI were determined to be 2.64, 2.60, 1.86, 1.88, and 1.77 eV, respectively. The substantial reduction in the E
g of the SA-g-CN/BiOI heterojunction suggests a synergistic interplay between the electronic and optical properties of SA-g-CN and BiOI, potentially contributing to enhanced photo(electro)catalytic activities.
The electrochemical properties of the semiconductor materials were characterized through Mott–Schottky analysis (
Figure 4c–e) in the presence of 0.1 M Na
2SO
4. The flat-band potential (E
fb) of the semiconductor materials can be determined using the Mott–Schottky plot (1/C
2 vs. potential) by extrapolating the linear portion to the point where it intercepts the X-axis (V
fb + kT/e) (Equation (2)). This E
fb value also corresponds to the Fermi level since band bending becomes negligible at the E
fb potential. In n-type and p-type semiconductors, the Fermi level aligns with the conduction band (E
cb) and valence band (E
vb) edges, respectively [
33].
Mott–Schottky analysis revealed flat band potentials (E
fb) of –1.27, –1.11, and –1.28 V for g-CN, SA-g-CN, and BiOI, respectively. Valence band potentials (E
vb) were subsequently calculated using Equation (3), resulting in values of +1.33, +1.53, and +0.58 V, respectively. Based on the determined E
g, E
cb, and E
vb values from DRS-Tauc and Mott–Schottky analyses, the corresponding band energy diagrams are presented in
Figure 4f.
Photoluminescence (PL) spectroscopy was employed to investigate charge carrier dynamics, specifically photoexcitation and recombination processes (
Figure 5a). Pristine g-CN exhibited an emission peak centered at approximately 475 nm, while sulfonic acid-functionalized SA-g-CN displayed a blue-shifted emission at around 445 nm. PL emission intensity is directly correlated with the rate of charge carrier recombination during photocatalytic and photoelectrochemical processes. Notably, g-CN/BiOI and SA-g-CN/BiOI composites demonstrated significantly reduced PL intensities compared to their pristine counterparts, indicating suppressed charge recombination due to the formation of heterojunction interfaces. This phenomenon is anticipated to contribute to enhanced photoelectrochemical performance.
The photocatalytic performance of the SA-g-CN/BiOI heterojunction catalyst was evaluated by monitoring the degradation of tartrazine (TTZ), a synthetic food dye, under simulated solar light irradiation (300 W Xenon lamp, AM 1.5G filter, 100 mW/cm
2). Approximately 0.02 g of catalyst was dispersed in 100 mL of a 10 mg/L TTZ aqueous solution. Prior to irradiation, the mixture was stirred in the dark to establish adsorption–desorption equilibrium. The progress of TTZ degradation was monitored via UV-Vis spectroscopy at 10 min intervals.
Figure 5b presents the TTZ concentration as a function of irradiation time (C/C
0), revealing a 98.26% removal efficiency within 60 min. This represents a 3.06, 2.14, 4.48, 1.56, and 16.48-fold enhancement compared to pristine g-CN (32.09%), SA-g-CN (45.91%), BiOI (21.9%), g-CN/BiOI (62.65%), and photolysis (32.09%), respectively. The superior photocatalytic activity of SA-g-CN/BiOI is attributed to a synergistic effect between SA-g-CN and BiOI. The sulfonic group acts as an electron trap, promoting electron transfer to the catalyst surface and extending the lifetime of charge carriers. Moreover, the formation of a heterojunction interface effectively suppresses charge recombination, thereby enhancing overall photocatalytic efficiency.
The kinetics of TTZ photodegradation was assessed by plotting –ln(C/C
0) against degradation time (t) (
Figure 5c). The linear relationship observed for the SA-g-CN/BiOI system indicates pseudo-first-order reaction kinetics, conforming to the equation –ln(C/C
0) = kt. The calculated rate constants (k) for TTZ photodegradation in the presence of various catalysts are presented in
Figure 5d. SA-g-CN/BiOI exhibited the highest rate constant (0.0534 min
−1), surpassing those of g-CN (0.00549 min
−1), SA-g-CN (0.00811 min
−1), BiOI (0.00322 min
−1), and g-CN/BiOI (0.0132 min
−¹). Importantly, all systems demonstrated excellent correlation coefficients (R
2) of unity, further supporting the pseudo-first-order kinetic model.
Electrochemical impedance spectroscopy (EIS) and transient photocurrent (TPC) measurements were employed to investigate charge transfer resistance (R
ct) and transient photoresponse, respectively. EIS spectra (
Figure 6a) revealed a significantly lower R
ct value of 9.1 Ω for SA-g-CN/BiOI compared to g-CN (44.5 Ω), SA-g-CN (15.1 Ω), BiOI (50.6 Ω), and g-CN/BiOI (90.2 Ω). The reduced R
ct in SA-g-CN/BiOI is attributed to efficient charge transfer facilitated by the heterojunction interface and the electron-trapping capability of the sulfonic group, promoting facile charge transport across the photoanode–electrolyte interface, and enhancing photoelectrochemical (PEC) performance. TPC measurements (
Figure 6b) were conducted via chronoamperometry (i-t) in 0.1 M NaOH under intermittent light conditions (10 s on/off cycles) to evaluate charge carrier dynamics. The SA-g-CN/BiOI nanocomposite exhibited the highest photocurrent response, corroborating the formation of an efficient heterojunction and the suppression of charge recombination.
The photoelectrochemical (PEC) water oxidation performance of the catalysts was assessed via linear sweep voltammetry (LSV) to evaluate oxygen evolution reaction (OER) activity.
Figure 6c presents LSV polarization curves recorded in 0.1 M Na
2SO
4 electrolyte containing Na
2SO
3 as a hole scavenger under simulated AM 1.5G illumination. A discernible enhancement in photocurrent was observed for all catalysts compared to their respective dark currents. Notably, the SA-g-CN/BiOI heterojunction exhibited the highest photocurrent density of 6.04 mA, surpassing those of g-CN (4.92 mA), SA-g-CN (5.47 mA), BiOI (2.54 mA), and g-CN/BiOI (4.1 mA). Moreover, the SA-g-CN/BiOI Z-scheme system demonstrated a lower onset potential of 0.94 V at a current density of 5 mA compared to the other catalysts. A comparative summary of photocurrent densities for all materials is provided in
Figure 6d. The formation of a Z-scheme heterojunction interface between SA-g-CN and BiOI is pivotal in augmenting photocatalytic efficiency. This interfacial region serves as an effective charge separation center, mitigating recombination losses and prolonging the lifetime of photogenerated charge carriers.
The recyclability of the SA-g-CN/BiOI Z-scheme composite was assessed through five consecutive photocatalytic degradation cycles of TTZ (
Figure 7a). A slight decrease in degradation efficiency from 98.31% to 93.24% was observed after the fifth cycle, primarily attributed to catalyst loss during recovery. Nevertheless, the overall retention of 93.24% degradation efficiency underscores the robust photocatalytic stability of the composite. To elucidate the dominant reactive species involved in TTZ degradation, radical trapping experiments were conducted using silver nitrate (SN), triethanolamine (TEOA), acrylic acid (AA), and isopropanol (IPA) as scavengers for electrons (e
−), holes (h
+), superoxide radicals (•O
2−), and hydroxyl radicals (•OH), respectively (
Figure 7b). The addition of AA resulted in a significant reduction of degradation efficiency to 51.72%, indicating that superoxide radicals (•O
2−) play a predominant role in TTZ removal, followed by holes (h
+), hydroxyl radicals (•OH), and electrons (e
−).
To assess the crystalline and chemical stability of the recycled catalysts, X-ray diffraction (XRD) and Fourier-transform infrared (FTIR) spectroscopy were employed.
Figure S2a presents the XRD patterns of the recycled SA-g-CN/BiOI nanocomposite catalyst after five successive reaction cycles, demonstrating excellent crystalline stability.
Figure S2b shows the FTIR spectrum of the recycled catalyst, indicating minimal changes in the chemical composition, thus confirming its robust chemical stability. These findings collectively suggest that the as-synthesized SA-g-CN/BiOI photocatalytic heterojunction exhibits remarkable stability under repeated reaction conditions. The structural integrity of the recycled SA-g-CN/BiOI heterojunction catalyst was assessed via FESEM analysis (
Figure S3a,b), which confirmed the preservation of the composite’s morphology and structural stability after five consecutive catalytic cycles. This observation underscores the catalyst’s robust nature and its potential for long-term application.
The photodegradation of TTZ was evaluated under varying pH conditions (
Figure 7c). The results indicate that TTZ photodegradation decreased with increasing pH from 3 to 11. At pH 3, a maximum TTZ photodegradation of 97.89% was achieved, while photodegradation decreased to 95.86% at pH 5. For pH 7, 9, and 11, TTZ removal percentages were 33.61%, 14.36%, and 13.58%, respectively. These findings suggest that TTZ adsorption onto the SA-g-CN/BiOI catalyst surface is enhanced at lower pH values due to increased protonation, leading to stronger electrostatic interactions. Conversely, at higher pH values, the decrease in protonation reduces TTZ adsorption, resulting in lower photodegradation efficiency.
A proposed photo(electro)catalytic mechanism for the SA-g-CN/BiOI heterojunction is illustrated in
Figure 7d. Bandgap energies (E
g), conduction band (CB), and valence band (VB) potentials (E
cb and E
vb) were determined through DRS and Mott–Schottky measurements. Calculated E
cb and E
vb values for SA-g-CN were −1.11 V and +1.53 V, respectively, while those for BiOI were −1.28 V and +0.58 V. Notably, the CB of SA-g-CN is positioned at a less negative potential compared to that of BiOI, while its VB is situated at a more positive potential.
Upon light irradiation, photogenerated electrons in the CB of SA-g-CN migrate to the VB of BiOI, recombining with holes. Consequently, electrons accumulate in the CB of BiOI, while holes concentrate in the VB of SA-g-CN. This spatial separation of charge carriers effectively inhibits recombination, promoting their participation in redox reactions. The observed Z-scheme charge transfer mechanism within the SA-g-CN/BiOI heterojunction is instrumental in enhancing photocatalytic and photoelectrochemical performance.
3. Materials and Methods
3.1. Materials
Dicyandiamide (C2H4N4 ≥ 99%), sulfuric acid (H2SO4 ≥ 99.999%), bismuth nitrate pentahydrate (Bi(NO3)3 · 5H2O ≥ 99.999%), potassium iodide (KI ≥ 99.0%), polyvinyl pyrrolidine (PVP-10,000 MW), methanol (CH3OH ≥ 99.8%), isopropanol (C3H8O ≥ 99.5%), silver nitrate (AgNO3 ≥ 99.999%), acrylic acid (C3H4O2 ≥ 99%), triethanolamine (TEOA ≥ 98%), sodium sulfate (Na2SO4 ≥ 99.0%), sodium sulfite (Na2SO3 ≥ 98.0%), sodium hydroxide (NaOH ≥ 97.0%), potassium chloride (KCl ≥ 99.0%), potassium ferri/ferrocyanide (K3[Fe(CN)6] ≥ 99.0%/K4[Fe(CN)6]·3H2O ≥ 98.5%), tartrazine (C16H9N4Na3O9S2 ≥ 85%), and Nafion (C7HF13O5S.C2F4 5 wt.%) were obtained from Sigma-Aldrich, Darmstadt, Germany, and used without further purification. Distilled water (DI) was used as a solvent throughout the reaction or otherwise stated.
3.2. Instrumentations and Characterizations
The phase composition and crystallographic structure of the prepared samples were confirmed by X-ray diffraction (XRD) analysis (Cu Kα radiation, λ = 1.5406 Å, PANalytical X’pert Pro, EA Almelo, The Netherlands). The chemical functional groups and bonding were analyzed through Fourier-transform infrared spectroscopy (FT-IR) with KBr pellets and a resolution of 4 cm−1 (PerkinElmer, Buckinghamshire, PA, USA), and X-ray photoelectron spectroscopy (XPS, JEOL-JPS-9030, Tokyo, Japan) with standard Mg source. The morphology, microstructure, and elemental composition were examined by field-emission scanning electron microscopy (FE-SEM, JEOL-JSM-7610F, Tokyo, Japan) equipped with energy-dispersive X-ray spectroscopy (EDX, X-MaxN, Oxford Instruments, Abingdon, UK). Optical properties were assessed through UV-visible diffuse reflectance spectroscopy (UV-DRS, Jasco V-770, Tokyo, Japan) and photoluminescence spectroscopy (PL, Micro PL-UniNanoTech, Gyeonggi-do, Republic of Korea) using 266 nm laser excitation. Electrochemical properties were studied via linear sweep voltammetry (LSV), electrochemical impedance spectroscopy (EIS), and Mott–Schottky analysis (Autolab PGSTAT128N-FRA32M, Livonia, MI, USA).
3.3. Synthesis of Pristine g-C3N4 (g-CN) and Sulfonic acid-Functionalized g-C3N4 (SA-g-CN)
The graphitic carbon nitride (g-CN) was synthesized by a thermal polycondensation reaction using dicyandiamide as a precursor material. Briefly, 4 g of dicyandiamide was placed in a silica crucible with the lid after being finely ground and heated in a muffle furnace at 550 °C for 3 h with a heating ramp of 5 °C/min. The pale-yellow g-CN was obtained and stored for further reactions. Secondly, 1 g of bulk g-CN was added to the glass bottle containing 0.1 M H2SO4 and stirred at 50 °C until all the solvents were evaporated by the total solvent evaporation (TSE) technique. Later, the obtained powder was heated at 200 °C for 2 h to strengthen the N–SO3H bond and SA-g-CN was obtained for further applications.
3.4. Synthesis of Pristine BiOI, g-CN/BiOI and SA-g-CN/BiOI Nanocomposites
The solvothermal method was employed for the synthesis of BiOI nanoplates. A volume of 100 mmol of Bi(NO3).6H2O and 0.2 M of potassium iodide was added to 1:1 ethylene glycol and distilled water mixture (80 mL) and stirred vigorously until the homogenous mixture was obtained. After that, the homogenous solution was added to the Teflon-lined autoclave and placed in the muffle furnace at 140 °C for 10 h. The obtained product was washed with DI and ethanol multiple times and dried overnight in a hot-air oven at 60 °C.
The nanocomposites were prepared by the total solvent evaporation (TSE) technique, and for this, equal amounts of g-CN, SA-g-CN and BiOI were added to the bottle containing 10 mL of methanol and kept for magnetic stirring at 60 °C until thorough solvent vaporization. Then, the obtained g-CN/BiOI and SA-g-CN/BiOI were dried overnight in a hot-air oven and utilized for further analyses and applications.
3.5. Photo(electro)chemical Measurements and Photocatalytic Applications
The photocatalytic oxidation of tartrazine (TTZ) was performed using pristine and composite materials. All the degradation reactions were carried out using a 350 W Xenon arc lamp with AM 1.5G filter (100 mW/cm2) obtained from Enlitech (ALS-300-G2), Taiwan, and the photoreactor was placed vertically about 40 cm from the light source. In this study, for the photocatalytic oxidation of TTZ dye, 50 mL (0.010 g L−1) was added with 25 mg of catalyst and bath-sonicated for even dispersion of the photocatalyst. The photocatalytic reactor was made of a double-walled Pyrex beaker with a water circulatory system to retain the optimum temperature throughout the experiment (24 ± 1 °C). After 15 min under stirring in dark conditions, the reactor was placed in the light source and the 3 mL aliquots were collected at regular intervals to determine the percentage of degradation using a UV-Vis spectrophotometer.
The Mott–Schottky plots were measured using a Metrohm Autolab potentiostat/galvanostat (FRA32M module integrated with NOVA). The electrochemical impedance spectroscopy (EIS) and the transient photocurrent (TPC) measurements were obtained using the electrochemical workstation (CHI1205B). For the Mott–Schottky measurements, 0.1 M Na2SO4 was used as an electrolyte. And for the photocurrent and EIS measurements, 0.1 M NaOH and 5 mM [Fe(CN)6]3−/4− mixture dispersed in 100 mM KCl were used as electrolyte solutions, respectively. In these analyses, Ag/AgCl (sat. KCl), a platinum wire, and a sample-coated indium tin oxide (ITO) plate were used as reference, counter, and working electrodes, respectively. The working electrode was prepared by cleaning the required ITO plates using acetone, ethanol, and deionized water, followed by drop casting the 50 µL of sample solution (i.e., 5 mg of photocatalysts dispersed in 1 mL DI/IPA mixture). The photo(electro)chemical oxygen evolution reactions (OER) were carried out using the same three-electrode system using 0.1 M Na2SO4/0.1 M Na2SO3 as the electrolyte solution.