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Photocatalytic degradation of methylene blue by Nd-doped titanium dioxide thin films

  • Liu Guodong , Mamatrishat Mamat EMAIL logo , Fuerkaiti Xiaerding and Wang Zhen
Published/Copyright: September 6, 2024
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Abstract

In this work, Nd (0.5, 1.0, 1.5, and 2.0 at%)-doped TiO2 thin films were synthesized on Si (100) substrates using a sol–gel spin-coating technique. The formation of the anatase phase was demonstrated by X-ray diffraction and Raman spectroscopy. It was also demonstrated that the doping of the Nd element resulted in a TiO2 crystal structure. X-ray photoelectron spectroscopy proved that the doping of Nd element promoted the transfer of Ti4+ to Ti3+, which facilitates the photocatalytic performance of the TiO2 films. Scanning electron microscope and atomic force microscope demonstrated that all of the Nd-doped film surfaces showed different degrees of aggregation relative to the pure TiO2 film surface. It was verified that the doping of Nd altered the lattice structure of TiO2 thin films, resulting in lattice defects on the surface and changing the grain size of the films. Meanwhile, the lattice defects and changes in the chemical state affect the photocatalytic performance of TiO2 films, and the highest photoactivity was observed for an Nd doping concentration of 1.0 at%. Nd doping causes lattice defects conducive to the formation of more Ti3+ oxidation centers and reduces the photogenerated electron–hole recombination rate, resulting in the improved photocatalytic performance of TiO2 films.

1 Introduction

Industrial production generates a large amount of industrial effluent, which contains a large number of chemicals that are harmful to the environment and the human body [1,2]. General methods of sewage treatment cannot deal with this chemical substance, and some treatment methods also produce secondary pollution. Photocatalytic technology is an emerging, efficient, and energy-saving modern green technology that decomposes pollutants into non-toxic or less toxic substances by using light radiation under the action of a catalyst. At present, the semiconductor photocatalysts that are widely studied basically belong to wide-band n-type semiconductor oxides, and more than ten types of photocatalysts have been studied, such as TiO2 [3], ZnO [4,5], CdS [6], WO3 [7], Fe2O3 [8], SnO2 [9], Cu2O [10], and SiO2 [11]. All of these semiconductor oxides have a certain degree of photocatalytic degradation of organic matter; however, because most of the semiconductor oxide materials are prone to chemical or photochemical corrosion, they are not suitable to be used as photocatalysts for wastewater treatment, while TiO2 is widely used for its excellent catalytic performance, stable chemical performance, safety, non-toxicity, no side-effects, a long time of persistence, and so on. This makes TiO2 one of the most potential photocatalysts for current applications. However, the characteristics of TiO2’s wider forbidden bandwidth (band gap = 3.2 eV) and relatively high carrier recombination rate severely limit its photocatalytic activity [12,13]. In order to improve the photocatalytic activity of TiO2, researchers have made numerous attempts to improve the photocatalytic activity of TiO2 by doping TiO2 compounds with metals and non-metals [14,15,16,17].

Currently, rare earth element doping is one of the common methods to improve the photocatalytic performance of TiO2 thin films. This is due to the unique electronic structure of the rare earth elements, where the electrons in the 4f orbitals are shielded by the electrons in the 5s and 5p orbitals, thus stabilizing the domains in the atomic structure. Meanwhile, the energy levels of the outer 4f and 5d orbitals together form the conduction band. The special domain and the non-full filled 4f electronic structure allow the rare earth elements to possess optical and magnetic properties that are very different from those of other metallic and non-metallic elements. Due to the above properties, the rare earth elements of La [18], Er [19], Yb [20], Sm [21], Eu, Ce [22], Pr, Nd [23], and Gd [24] have been used to improve the photocatalytic activity of semiconductor oxides.

Regarding the thin film fabrication, the sol–gel, electrostatic spinning, magnetron sputtering, co-precipitation, complexation, and spray pyrolysis methods have been used for the deposition of TiO2 thin films. The sol–gel method is one of the most dominant techniques for the large-scale synthesis of thin films due to the advantages of low cost, short preparation cycle, and ease of large-scale industrialization [25]. Meanwhile, the solution coating method is a film-making technology that does not require a vacuum environment and has been widely used in microelectronic devices and surface coating because of the small size of the required equipment, the ability of film formation on the surface of a variety of substrates, and the ease of solving raw materials. Therefore, it is considered one of the common methods for TiO2 film preparation.

Among all the rare earth elements, Nd has been less studied; especially, the mechanism and optical properties need further study systematically. In addition, some studies in this field have shown that Nd has a great potential application in improving the photocatalytic degradation properties, such as transmission and absorption of TiO2 [26,27,28,29]. Therefore, the aim of our work is to synthesize TiO2 thin films using a cost-effective sol–gel spin-coating technique, to investigate the effect of Nd dopants on the structural, optical, and photocatalytic properties of TiO2 and to explore its application in wastewater treatment. For the Nd-doped TiO2 films, first, the crystal structure and surface morphology were examined, the optical properties were then studied, and finally, the photocatalytic activity for methylene blue (MB) degradation under artificial sunlight irradiation was investigated, and the possible mechanism was explained.

2 Experimental procedure

2.1 Preparation of thin films

The Nd-doped TiO2 films were prepared using the sol–gel method. A 0.2 M TiO2 solution was used with butyl titanate (Sigma Aldrich 99%), acetylacetone (Merck 99%), hydrochloric acid (Merck 37%), polyethylene glycol-2000, and neodymium(iii) nitrate hexahydrate (99.9%). Two solutions (solution A and solution B) were prepared in the first step. About 5 mL of butyl titanate (0.02 mol) was mixed with 20 mL of anhydrous ethanol and 1.5 mL of acetylacetone (0.015 mol) to prepare solution A. Solution B was prepared from 15 mL of anhydrous ethanol and 2 mL of deionized (0.11 mol) water. Then, solution A and solution B were stirred separately for 20 min, and then were mixed and stirred, and the pH of the solution was adjusted to about 1–2 with HCl. Afterward, polyethylene glycol (PEG-2000) 0.3 g (0.00016 mol) was added to increase the dopant ratios to 0.5, 1.0, 1.5 at%, and 2.0 at% Nd/Ti in the TiO2 precursor solution, and the final solution was subjected for hydrolytic condensation reaction for 24 h. Next, the cleaned silicon wafer as substrate (single-polished p-type (100) crystal direction, with a thickness of 725 μm ± 10 μm, size of 20 mm × 20 mm) was placed in a suction cup of the screeding machine, and the precursor solution was dripped on the silicon wafer and the spin coating was started with a low speed of 1,000 rpm and then at a high speed of 3,000 rpm. After spin-coating, the spin-coated sample was heated at 100°C for 5 min. Then, the above procedures were repeated 20 times. The spin-coated samples are then annealed under a nitrogen atmosphere. The homogenized spin-coated sample was placed in a high-temperature tube furnace (OTF-1200). The program was set to increase the temperature by 5°C every minute, and the final temperature was set to 700°C. After reaching the holding temperature, the temperature was maintained at 700°C for 30 min and then cooled naturally. Before thermal annealing, the tube was vacuumed to about −0.02 Pa, and then nitrogen gas was passed to the tube to about 0.04 Pa. The above steps were repeated two to three times, and then the gas flow meter (D08-3E) was turned on to adjust the gas flow rate to 120 cm3. The flow rate of the gas remained unchanged until the end of the annealing process. The sample preparation procedure is shown in Figure 1. For the transmission spectra measurement, the Nd-doped TiO2 samples were fabricated on the glass substrate, keeping all the conditions same as above.

Figure 1 
                  Thin film preparation process.
Figure 1

Thin film preparation process.

2.2 Characterization

After deposition, the necessary characterization was carried out to explore the physical properties of the TiO2 films. The crystal structure of the films was investigated using a Bruker D8 Advance X-ray diffractometer (XRD) (λ = 1.54 Å), Germany. The X-ray data of all the samples were recorded at a scanning speed of 2°/min between 20° and 60°. The thin film lattice structure of the films was also investigated using a Renishaw inVia Reflex Raman spectrometer (UK). The laser was selected to be 532 nm with a beam range of 100–3,500 cm−1. Changes in the chemical state of the films were investigated using a Thermo Fisher Scientific ESCALAB250Xi X-ray photoelectron spectrometer (USA). The surface morphology of the films was investigated using a Hitachi su8010 field emission scanning electron microscope (FESEM). The surface roughness of the thin films was investigated using a Bruker Dimension ICON atomic force microscope. Transmission spectra were obtained at room temperature using a LAMBDA 650 PerkinElmer UV-Vis spectrophotometer in the wavelength range of 200–800 nm.

2.3 Photocatalytic activity measurement

The photocatalytic activity of TiO2 films was investigated by determining the degradation of aqueous solutions of MB under visible light irradiation. MB, with a concentration of 5 mg/L was selected as a non-biodegradable organic pollutant in this study. The photocatalytic experiments were carried out in glass test tubes at room temperature. First, the adsorption–desorption equilibrium was established by the solution that was left in the dark for 30 min before light irradiation. Then, TiO2 films were immersed in MB solution, and the aqueous solution in the beaker was irradiated using a xenon lamp with a power of 350 W, where the xenon lamp light source was kept 10 cm above the beaker. The concentration of MB in the solution was monitored by collecting 4 mL of the irradiated solution every 2 h and recording the intensity of the UV-visible absorbance peaks as a function of reaction time:

(1) η = C 0 C / C 0 × 100 % = A 0 A / A 0 × 100 % ,

where C 0 and A 0 are the initial concentration and absorbance of MB solution at 664 nm, respectively, and C and A are the concentration and absorbance of MB solution at 664 nm under UV irradiation at different times, respectively. The blank and dark experiments were corrected as the perturbations generated by the UV-vis radiation and film adsorption, respectively.

3 Results and discussion

3.1 XRD pattern analysis

Figure 2 shows the XRD patterns of the undoped and Nd-doped TiO2 thin film samples annealed at 700°C. The XRD curve of the undoped TiO2 thin film sample (curve a) at 2θ = 25.30, 37.79, and 48.03° corresponds to a TiO2 thin film with tetragonal geometry. The peaks match well with the card (JCPDS 84-1286). The peaks at 2θ = 27.44, 44.04, and 56.63° correspond to the rutile phase of TiO2 films (JCPDS-86-0148). Similar peaks are also observed in the XRD curve of the Nd-doped sample (b–e).

Figure 2 
                  XRD spectra of the TiO2 film with Nd doping.
Figure 2

XRD spectra of the TiO2 film with Nd doping.

Compared to the undoped TiO2 thin film samples with Nd-doped samples, the diffraction intensity of the anatase diffraction peaks that decrease gradually can be observed, and the sharp peak pattern was changed to the dull peak pattern. Some of the diffraction peaks of the anatase phase almost disappeared in the TiO2 thin film sample, which was doped with 2% (curve e). The change in the diffraction peaks of the rutile phase with the increase of the doping ratio is exactly opposite to the change in the diffraction peaks of the anatase phase. The results indicate that doping leads to the deterioration of the crystallinity of the anatase phase and promotes the transformation of TiO2 from the anatase phase to the rutile phase. Meanwhile, we did not find any additional diffraction peaks that belong to the Nd elements or the related compounds and oxides, which can be attributed to the low percentage doping ratio or to indicate only a small amount of Nd3+ entering the TiO2 lattice instead of Ti4+ [30].

The crystallite size of the sample was calculated from the Scherrer equation (equation (2)) by selecting the diffraction peaks at the crystal plane (101) in the data analysis [31]:

(2) D = K γ β cos θ ,

where D is the average thickness of the grain that is in the direction perpendicular to the grain plane (Å), K is the Scherrer coefficient (K = 0.89 if β is the half-peak height and width of the diffraction peak, and K = 1 if β is the integral height and width of the diffraction peak), θ is the Bragg angle, γ is the X-ray wavelength with a value of 1.54056 Å. The values of the crystallite size, cell parameters, and cell volume for all samples are given in Table 1. It can be noted from the table that the grain size of the doped samples decreased as compared to the undoped samples. The values of the cell parameters and lattice size are compared with each other between the doped samples, and the grain size decreases with an increase of the doping percentage. The results showed that the sample size with a doping rate of 2% is increased, which corresponds to the trend of the diffraction peak of the 25.30° (101) anatase phase [31,32,33,34,35,36,37,38,39].

Table 1

Cell parameters and lattice size values of undoped and doped TiO2 films

Samples Crystallite size (nm) FWHM a = b(Å) c(Å) c/a
TiO2 37.9 0.239 3.780 9.510 2.516
At 0.5% Nd-TiO2 29.6 0.306 3.777 9.501 2.515
At 1.0% Nd-TiO2 26.9 0.337 3.776 9.486 2.512
At 1.5% Nd-TiO2 14.6 0.652 3.747 9.486 2.512
At 2.0% Nd-TiO2 24.2 0.392 3.776 9.486 2.512

3.2 Raman profiling

Figure 3 shows the Raman spectra of the undoped TiO2 film and the doped TiO2 film with different doping ratios. With reference to the labeled Raman spectrogram data of the undoped TiO2 crystals [40], the anatase phase of TiO2 has six Raman vibrational modes: A1g + 2B1g + 3Eg, corresponding to the Raman peaks at 519 cm−1 (A1g + 2B1g, ν1 + ν2), 399 cm−1 (B1g, ν3), 640 cm−1 (Eg, ν4), 199 cm−1 (Eg, ν5), and 144 cm−1 (Eg, ν6). The rutile phase TiO2 has four Raman vibrational modes: A1g + B1g + B2g + Eg, corresponding to Raman peaks of 612 cm−1 (A1g, ν1), 143 cm−1 (B1g, ν2), 826 cm−1 (B2g, ν3), and 447 cm−1 (Eg, ν4) [14]. As shown in Figure 3, the deposited TiO2 films and their doped films on the silicon wafer substrate show obvious characteristic peaks of anatase and rutile phases, which are consistent with the XRD results. According to the literature, the vibrational peaks of anatase TiO2 in the Raman spectra represent the symmetric stretching vibrations, the symmetric bending vibrations, and the antisymmetric bending vibrations of the O–Ti–O bond, therefore reflecting the corresponding Eg, B1g, and A1g vibrational modes in the spectra [41]. The Eg mode is sensitive to the motion of the oxygen sub-lattice, the B1g mode is dominated by the Ti motion, and the A1g mode is also dominated by the same but opposite mode (antisymmetric). Since the Eg mode is particularly sensitive to the oxygen vacancy (Ov) defects, the variation of the Eg vibrational modes can be recognized as a direct indication of the presence of intrinsic defects in anatase TiO2 [42]. The Eg modes are sensitive to the motion of the oxygen sub-lattice, with the B1g mode dominated by Ti motion and the A1g mode dominated by the same but opposite mode (antisymmetric). As the Eg mode is particularly sensitive to Ov defects, changes in the Eg vibrational mode can be considered a direct indication of the presence of intrinsic defects in the anatase TiO2. Analysis of the spectrum in Figure 3 shows peaks at 144, 301, 399, 447, 525, and 639 cm−1. Since the silicon wafer was used as the substrate for the experiment, the 301 and 525 cm−1 peaks in the spectra represent the Raman peaks of SiO2 and Si, respectively. Therefore, the two peaks are not used as the object of analysis in the study. From the above Raman spectra, 144, 399, and 639 cm−1 in the spectrum represent the anatase phase, and 447 cm−1 represents the rutile phase. Since the peaks at 399, 447, and 639 cm−1 do not vary as much when compared to the 144 cm−1 peak, thus the main analysis is on the Eg 144 cm−1 peak. At the different doping ratios, the main Eg peaks of TiO2 films show no significant peak shift but the different changes in the intensity under the effect of the doping element Nd (Figure 3a). When the doping ratio reaches 0.5 at% (Figure 3b), the vibrational peak intensity of the main Eg peak decreases relative to that of the undoped sample. As the doping ratio continues to increase, the intensity of the main Eg peak increases, and reached at a maximum at 1.5 at% (Figure 3d) and decreased again at 2.0 at% (Figure 3e). The trend of the anatase phase in the Raman spectra is consistent with the trend of the anatase phase in the XRD spectra, which proves that a large number of crystal defects are generated in the crystal due to Nd doping, leading to a decrease in the crystallinity of the TiO2 film. As the position of the peaks in Figures 2 and 3 does not change significantly, the intensity of the peaks changes with the doping ratio and the corresponding trend [43]. The doping of Nd changes the long-range symmetric ordered structure of the TiO2 lattice to disordered (disordered structure can be shown in Section 3.4) [44]. The introduction of the dopant Nd also leads to the formation of defects in the Ti–O structure, which are explained in Section 3.3 [45,46,47,48].

Figure 3 
                  Raman spectra of the TiO2 films: (a) undoped film, (b), (c), (d), and (e) are the films doped with Nd at 0.5, 1.0, 1.5, and 2.0%, respectively.
Figure 3

Raman spectra of the TiO2 films: (a) undoped film, (b), (c), (d), and (e) are the films doped with Nd at 0.5, 1.0, 1.5, and 2.0%, respectively.

3.3 X-ray photoelectron spectroscopy (XPS) pattern analysis

XPS can be used to analyze the changes in the chemical states of the elements of interest in a sample. In this study, the chemical states of Nd, Ti, and O were analyzed in all samples. All data analyses were calibrated against a peak of 284.80 eV for C 1s in element C as a standard peak. The measured spectral data of the sample films are shown in Figures 47.

Figure 4 
                  X-ray photoelectron spectra of the TiO2 thin film: (a) chemical state of O and (b) chemical state of Ti.
Figure 4

X-ray photoelectron spectra of the TiO2 thin film: (a) chemical state of O and (b) chemical state of Ti.

Figure 5 
                  X-ray photoelectron spectra of Nd: (a) doped at 0.5% Nd-TiO2 film, (b) doped at 1.0% Nd-TiO2 film, (c) doped at 1.5% Nd-TiO2 film, and (d) doped at 2.0% Nd-TiO2 film.
Figure 5

X-ray photoelectron spectra of Nd: (a) doped at 0.5% Nd-TiO2 film, (b) doped at 1.0% Nd-TiO2 film, (c) doped at 1.5% Nd-TiO2 film, and (d) doped at 2.0% Nd-TiO2 film.

Figure 6 
                  X-ray photoelectron spectra of Ti: (a) doped at 0.5% Nd-TiO2 film, (b) doped at 1.0% Nd-TiO2 film, (c) doped at 1.5% Nd-TiO2 film, and (d) doped at 2.0% Nd-TiO2 film.
Figure 6

X-ray photoelectron spectra of Ti: (a) doped at 0.5% Nd-TiO2 film, (b) doped at 1.0% Nd-TiO2 film, (c) doped at 1.5% Nd-TiO2 film, and (d) doped at 2.0% Nd-TiO2 film.

Figure 7 
                  X-ray photoelectron spectra of O: (a) doped at 0.5% Nd-TiO2 film, (b) doped at 1.0% Nd-TiO2 film, (c) doped at 1.5% Nd-TiO2 film, and (d) doped at 2.0% Nd-TiO2 film.
Figure 7

X-ray photoelectron spectra of O: (a) doped at 0.5% Nd-TiO2 film, (b) doped at 1.0% Nd-TiO2 film, (c) doped at 1.5% Nd-TiO2 film, and (d) doped at 2.0% Nd-TiO2 film.

Figure 4 exhibits the XPS spectra of the undoped TIO2 films for the elements O (a) and Ti (b). Figure 5 corresponds to the XPS spectra of Nd; from spectra (a–d), it can be seen that all samples have two diffraction peaks, Nd 3d3/2 and Nd 3d5/2, which are due to the spin–orbit splitting of Nd3+ ions, and the appearance of the diffraction peaks proves that all the samples have been successfully doped with Nd3+ ions. Figures 6 and 7 exhibit the XPS profiles of Ti and O elements for all doped samples.

The spectra corresponding to the Ti element are shown in Figure 6. From the spectra, it can be seen that the two diffraction peaks, Ti 2p1/2 and Ti 2p3/2, appear in the spectra of all samples [49]. The presence of two peaks from the spin-orbit splitting of the Ti ions proves the presence of the Ti ions in all samples. The positions of all of the peaks in the samples are listed in Table 2. A comparative study of the peaks for all of the samples shows no significant shift in the peak positions in the TiO2 film (Figure 4a) and all doped samples (Figure 6b–e) as the doping ratio of Nd ions increases. At the same time, it can be concluded from the shift of the peaks in the plots that the Ti3+-related defects are present in the samples. The charge mechanism regarding the formation of Ti3+, which is related to defects, is shown in equation (3) [50]:

(3) e CB + Ti 4 + Ti 3 + + trapped electron .

Table 2

Peak positions of Ti and O chemical states in XPS patterns

Samples O2 (eV) Ov (eV) −OH/H2O (eV) Ti4+ (eV) Ti3+ (eV)
TiO2 529.90 531.41 532.61 458.82 464.82 458.55 464.08
0.5 at% Nd-TiO2 529.79 531.42 532.71 458.76 464.66 458.35 463.95
1.0 at% Nd-TiO2 529.73 531.57 533.0 458.62 464.66 458.25 463.90
1.5 at% Nd-TiO2 529.55 531.38 532.57 458.67 464.57 458.30 463.90
2.0 at% Nd-TiO2 529.80 531.50 532.84 458.55 464.62 458.24 463.94

With the different doping ratios, the area under the peaks corresponding to Ti 2p changes correspondingly compared to the spectra of the undoped TiO2 films, and the area of the peaks related to Ti3+ of the Nd-doped samples increases with increasing doping ratios. The highest peak area reached 1.0% Nd doping and then decreased. The results are matched by the variation of Ti4+. In contrast to the trend of Ti3+, the height and area of the peaks decrease when the proportion of Nd doping increases, and they reach a minimum of 1.5%. The height of the peak increases again when the proportion of Nd doping is at 2.0%.

Figure 7 shows the O 1s spectra of the undoped and Nd-doped TiO2 films. The O 1s spectrum consists of three peaks, the first of which corresponds to the bonding of O2− to the saturated Ti4+ ion. The second peak corresponds to the detachment of oxygen atoms (oxygen ions) from the matrix lattice, resulting in the formation of vacancies due to oxygen deficiency. The third peak, located near 533 eV is composed of loosely bound oxygen adsorbed on the surface of the TiO2 attached to hydroxyl or water, and the interstitial oxygen may also interact with these hydrogen/hydroxyl groups [30]. After doping with Nd, the height of the first peak of O 1s is significantly increased when the sample is doped at 0.5% and becomes the highest peak of all samples. As the doping percentage increases, the change in the peak decreases. The trend is consistent with the trend of the peak and the fitted area of Ti4+. The second peak represents the change in Ov in the sample, and its trend is consistent with the peak of Ti3+ and the fitted trend [49,51].

All samples were annealed in a tube furnace under N2 atmosphere and in an oxygen-free environment. Therefore, the O elements that could be detected in the samples could not have been obtained from the reaction of the samples with oxygen in the air. In this oxygen-free high-temperature (700°C) environment, not only are Ti–O bonds formed, but the organic molecules present in the precursor solution that are spin-coated on the silicon wafer substrates cause the electrons on the hydrogen in the organic-OH to undergo electron transfer to the oxygen in the environment. Therefore, an Ov is formed. The presence of the Ovs causes a change in the chemical state of the element Ti, prompting the reduction of Ti4+ to Ti3+. This results in the presence of Ovs and Ti3+ chemical states in the pure TiO2 film samples. From the above analysis, with the addition of Nd ions, the Ov and Ti3+ chemical states also change. This result confirms the interaction between Nd and Ti in the titanium matrix, that the addition of Nd also reduces Ti4+ to Ti3+, and that Nd ions favor the generation of the Ovs in TiO2 films.

In the present study, the influencing factor is mainly the dopant ion, while the changes in the Ov and Ti3+ chemical state can be explained by the electronegativity of the dopant ion and the matrix. This is because the electrons in the energy level orbitals are subject to the strong Coulombic interactions of the nucleus and have a certain binding energy on the one hand, and to the shielding effect of the outer electrons on the other. When the density of the outer core electrons decreases, the shielding effect decreases and the binding energy of the inner core electrons increases. Conversely, the binding energy decreases. According to the electronegativity defined by Pauling, it is known that the electronegativity values of element Nd, element Ti and element O are 1.14, 1.54 and 3.44, respectively [52], and the electrons of the Nd atom are transferred to the titanium atom. This increases the electron density of the titanium atom, increases the shielding effect, and reduces the binding energy of the inner electrons. The electron density of the Nd atom decreases, the shielding effect is weakened, and the binding energy of the inner core electrons increases.

As a portion of Nd ions enter the TiO2 film lattice at high temperatures to substitute Ti ions, at the same time the valence band electrons of Nd atoms are transferred to Ti atoms due to electronegativity. In order to maintain charge neutrality, the increase of Ovs in the system is promoted. Therefore, Nd3+ can produce a change in the Ovs by breaking the local electrostatic equilibrium, replacing the position of the Ti ion, thus maintaining charge neutrality. Therefore, Nd–O–Ti valence bonds are formed in the lattice of the TiO2 films, and a stable lattice structure is produced. The surface morphology of the film changes as the doping ratio increases, and the ratio of Ti3+ to Ov also changes [53]. It is clear from the literature that the increase in Ti3+ and Ov improves the photocatalytic performance of the samples. The peak and ratio of Ti3+ and Ovs reach the maximum at a doping ratio of 1.0%. The performance of photocatalytic degradation in this study corresponds to Ti3+ and OVs. This also corresponds to the trend of (101) for the anatase phase in XRD and Eg (144 cm−1) in the Raman spectra, which is consistent with the above data analysis.

The Ov and Ti3+ defects were quantified using the following relationships (equations (4) and (5)), and the atomic concentrations of these defects are recorded in Table 3:

(4) [ O v ] = Area of O v Area of O v + Area of O 2 + Area of ( OH / H 2 O ) ,

(5) Ti 3 + = Area of Ti 3 + Area of Ti 3 + + Area of Ti 4 + .

Table 3

Area ratio of Ti and O chemical states in XPS patterns

Samples O2− (Conc.%) Ov (Conc.%) −OH/H2O (Conc.%) Ti4+ (Conc.%) Ti3+ (Conc.%)
TiO2 0.381 0.439 0.180 0.547 0.453
0.5 at% Nd-TiO2 0.680 0.218 0.102 0.631 0.369
1.0 at% Nd-TiO2 0.543 0.326 0.131 0.383 0.617
1.5 at% Nd-TiO2 0.472 0.387 0.141 0.404 0.596
2.0 at% Nd-TiO2 0.592 0.320 0.088 0.707 0.293

According to Figure 3 and Tables 2 and 3, it can be concluded that in the undoped sample, there are Ov and Ti3+ related defects in the sample due to the organic residues at high annealing temperatures and the electronegativity difference between Ti and O [54]. In the doped samples, the defects are enhanced due to the electronegativity difference between Ti and Nd. Ultimately, the electron migration in the valence band due to the electronegativity of the doped ions is more favorable to the increased Ov and Ti3+ states in the corresponding samples, and the Ov and Ti3+ states in the samples reduce the probability of recombination of holes with electrons, thus improving the photocatalytic degradation performance of the samples.

3.4 FESEM and AFM analysis

Figures 8 and 9 show the Scanning electron microscope (SEM) and atomic force microscope (AFM) images of the undoped and doped samples, which display the variation of surface morphology and surface roughness of the Nd-doped TiO2 films. Figure 8 demonstrates the uniform porous macrostructure of undoped TiO2 films (a). The surface morphology transforms to granular with protrusions when the doping ratio is gradually increased to at 0.5%. As the doping percentage increases, the morphology of the particles also changes. The particles start to aggregate when the doping is at 1.0% (c), and all particles agglomerate together when the doping is at 2.0% (e). Correspondingly, the morphological changes shown in Figure 5 are consistent with the demonstration by the SEM images.

Figure 8 
                  SEM images of (a) undoped TiO2 film, (b) doped 0.5 at% NdTiO2 film, (c) doped 1.0 at% Nd-TiO2 film, (d) doped 1.5 at% Nd-TiO2 film, and (e) doped 2.0 at% Nd-TiO2 film.
Figure 8

SEM images of (a) undoped TiO2 film, (b) doped 0.5 at% NdTiO2 film, (c) doped 1.0 at% Nd-TiO2 film, (d) doped 1.5 at% Nd-TiO2 film, and (e) doped 2.0 at% Nd-TiO2 film.

Figure 9 
                  AFM images of (a) undoped TiO2 film, (b) doped 0.5 at% NdTiO2 film, (c) doped 1.0 at% Nd-TiO2 film, (d) doped 1.5 at% Nd-TiO2 film, and (e) doped 2.0 at% Nd-TiO2 film.
Figure 9

AFM images of (a) undoped TiO2 film, (b) doped 0.5 at% NdTiO2 film, (c) doped 1.0 at% Nd-TiO2 film, (d) doped 1.5 at% Nd-TiO2 film, and (e) doped 2.0 at% Nd-TiO2 film.

Meanwhile, we can estimate the roughness variation of the sample using AFM, as shown in Table 4. According to the literature, there are four main modes of doped films, and some researchers believe that the ions of dopants may exist mainly in TiO2 with four forms: 1) one is aggregated to the surface of TiO2 in the form of crystallite of oxides; 2) one is stepped uniformly to the surface of TiO2 in the form of crystallite of oxides, 3) one is into the lattice gap of TiO2, and 4) substitution of Ti ions in the lattice [37,38,39,40,41,42]. Since the radius of the Nd3+ ion is much larger than that of TiO2, the doping of Nd ions changes the lattice structure of TiO2. As can be seen in Figures 8 and 9, the doping of Nd ions resulted in a large number of lattice defects in the lattice, changing the surface morphology of the films. The presence of the first or second form will mainly occur when Nd3+ is doped. Excess Nd3+ will eventually appear on the surface of the grains or at the grain boundaries. The dopant located at the grain boundaries hinders the interaction between the grains, increasing the dopant ratio, and the crystallinity of the anatase phase decreases instead of the crystallinity of the rutile phase increase. With the continued increase in the proportion of Nd doping (doping from 0.0 to 0.5 at%), neodymium ions do not continue to take the place of titanium ions in the titanium dioxide lattice. As the doping ratio continues to increase (doping from 0.5 to 2.0 at%), all Nd ions that cannot be substituted will accumulate on the surface of the film. This result is consistent with the change in the surface morphology as shown in the SEM images, while the change in the roughness of the sample as shown in e Table 4, and the trend is also consistent with the trend of the crystallite size in Table 1.

Table 4

Estimated roughness values of the samples from AFM

Samples TiO2 0.5 at% Nd 1.0 at% Nd 1.5 at% Nd 2.0 at% Nd
R a (nm) 7.870 1.830 1.270 0.567 0.990
R q (nm) 10.30 2.35 1.61 0.81 1.40
R max (nm) 73.5 28.6 17.0 13.8 19.1

3.5 Optical analysis

The UV-Visible transmission and absorption spectra of all the samples are shown in Figure 10(a) and (b), respectively, and the band gaps of the samples at different doping concentrations are shown in Figure 10(c). From the figure, it can be seen that Nd doping affects the intrinsic transmittance and intrinsic absorbance of TiO2. As shown in Figure 10(a), the position of the transmission fringes of the UV-Vis transmission spectra of the undoped and doped TiO2 films are shifted. The transmittance of the films increases with the gradual increase in the amount of doped Nd [33,34,55]. As can be seen from the figure, the transmittance of Nd-doped TiO2 films significantly increased in the 370–550 nm band region compared to the undoped TiO2 film [56,57,58]. It can be seen that the energy levels of TiO2 films with different doping levels are lower than those of pure TiO2 films in the region of 350–450 nm; from (b), it can be seen that the absorption edge of Nd-doped TiO2 films is blue-shifted [45,47]. The known intrinsic absorptivity data can be used to calculate the band gap of the sample by the intercept method. Based on the principle that the bandwidth Eg is inversely proportional to semiconductor absorption threshold λ g as follows:

E g ( eV ) = 1 , 240 / λ g ( nm ) .

Figure 10 
                  (a) Transmittance spectra of the sample with different doping concentrations. (b) Absorbance spectra of the sample for MB solution and (c) band gap of the sample with different doping concentrations.
Figure 10

(a) Transmittance spectra of the sample with different doping concentrations. (b) Absorbance spectra of the sample for MB solution and (c) band gap of the sample with different doping concentrations.

Therefore, Eg can be obtained through the acquisition of λ g. From the UV-vis DRS (UV-Vis diffuse reflectance) spectra, the wavelength–absorption curve is differentiated once, and then an intercept is made at the extreme point (the slope is the value of the longitudinal coordinate of the extreme point), and the intersection point of the intercept and the transverse coordinate is λ g. Substituting into the above equation, we can obtain the forbidden bandwidth of the material, i.e., E g. The calculated values of undoped, 0.5, 1.0, 1.5, and 2.0% Nd are 3.444, 3.599, 3.615, 3.573, and 3.553 eV, respectively. Based on the above data, the trend of the bandgap size is as follows: Nd-doped Nd 1.0 at% > 0.5 at% > 1.5 at% > 2.0 at% > TiO2. From the above analysis, it is known that the doping of the Nd element leads to an increase of the band gap. From Table 1, it is known that the doping of Nd ions leads to smaller lattice size, and from the theory of size quantum effect, it is known that the smaller the grain, the wider the band gap, and the larger the absorption band edge displacement. The doping of Nd ions reduces the size of the TiO2 crystallite. The reduction of the grain size makes the energy gap wider, which makes the valence band potential more positive, and the conduction band potential becomes more negative, which, in fact, increases the oxidation–reduction capacity of the photogenerated electrons and holes and improves the activity of the semiconductor photocatalytic degradation of the organic compounds.

Figure 11 shows the curves of the remaining percentage of Nd-doped TiO2 films degrading MB in the visible light as a function of time and examines the rate of MB degradation by the films over a period of 12 h. The Nd-doped TiO2 films also show a tendency to degrade MB faster and then slower. The highest degradation rate of 67.4% was achieved after 12 h when the Nd doping level was 1.0 at% of the sample. When the doping amount was higher than 1.0%, the degradation efficiency decreased instead, which was attributed to the fact that the excessive doping of Nd changed the film structure and reduced the photocatalytic efficiency instead. As can be seen from Figure 11, the results of the photocatalytic activity with doping amounts are 1.0 at% TiO2 > 0.5 at% TiO2 > 2.0 at% TiO2 > 1.5 at% TiO2 > TiO2. The results of photocatalytic performance are in agreement with the results of the data analyses in the above sections.

Figure 11 
                  Residual percentage of visible light degradation of MB by Nd-doped TiO2 films.
Figure 11

Residual percentage of visible light degradation of MB by Nd-doped TiO2 films.

4 Conclusion

In this work, the sol–gel method was used to prepare Nd3+ ion-doped TiO2 films, which were annealed at 700°C. The crystalline phase of the films was altered by doping of Nd ions, and the crystallinity was reduced. The surface morphology of the films was changed, and a large number of lattice defects were generated, which promoted the generation of a large number of Ti3+ oxidation centers. Meanwhile, the doping of Nd3+ ions reduces the crystallite size. This change in the physical properties of Nd-doped TiO2 films reduced the photogenerated electron–hole recombination rate and redox capacity, which greatly improved the photocatalytic performance of the TiO2 catalysts. The ability of MB degradation under artificial sunlight makes Nd-doped TiO2 film a potential material candidate for improving wastewater treatment.

Acknowledgments

Thin work was supported by the Natural Science Foundation (Grant No: 2021D01C037) and Special Training Program (Grant No: 2020D03001) of Science and Technology Department of Xinjiang, China.

  1. Funding information: This work was supported by the Natural Science Foundation (Grant No: 2021D01C037) and the Special Training Program (Grant No: 2020D03001) of the Science and Technology Department of Xinjiang, China.

  2. Author contributions: Liu Guodong performed characterization of optical properties (absorption spectra measurement and photocatalytic measurements). Mamatrishat Mamat supervised the whole work and reviewed and revised the manuscript. Fuerkaiti Xiaerding supervised the experimental work and was mainly responsible for XPS data analysis. He also reviewed and revised the manuscript. Wang Zhen supervised the experimental work and was mainly responsible for the Raman spectra measurement and data analysis. He also reviewed and revised the manuscript. All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors state no conflict of interest.

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Received: 2023-11-02
Revised: 2024-04-28
Accepted: 2024-07-10
Published Online: 2024-09-06

© 2024 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  45. Multicriteria-based optimization of roller compacted concrete pavement containing crumb rubber and nano-silica
  46. Revisiting hydrotalcite synthesis: Efficient combined mechanochemical/coprecipitation synthesis to design advanced tunable basic catalysts
  47. Exploration of irreversibility process and thermal energy of a tetra hybrid radiative binary nanofluid focusing on solar implementations
  48. Effect of graphene oxide on the properties of ternary limestone clay cement paste
  49. Improved mechanical properties of graphene-modified basalt fibre–epoxy composites
  50. Sodium titanate nanostructured modified by green synthesis of iron oxide for highly efficient photodegradation of dye contaminants
  51. Green synthesis of Vitis vinifera extract-appended magnesium oxide NPs for biomedical applications
  52. Differential study on the thermal–physical properties of metal and its oxide nanoparticle-formed nanofluids: Molecular dynamics simulation investigation of argon-based nanofluids
  53. Heat convection and irreversibility of magneto-micropolar hybrid nanofluids within a porous hexagonal-shaped enclosure having heated obstacle
  54. Numerical simulation and optimization of biological nanocomposite system for enhanced oil recovery
  55. Laser ablation and chemical vapor deposition to prepare a nanostructured PPy layer on the Ti surface
  56. Cilostazol niosomes-loaded transdermal gels: An in vitro and in vivo anti-aggregant and skin permeation activity investigations towards preparing an efficient nanoscale formulation
  57. Linear and nonlinear optical studies on successfully mixed vanadium oxide and zinc oxide nanoparticles synthesized by sol–gel technique
  58. Analytical investigation of convective phenomena with nonlinearity characteristics in nanostratified liquid film above an inclined extended sheet
  59. Optimization method for low-velocity impact identification in nanocomposite using genetic algorithm
  60. Analyzing the 3D-MHD flow of a sodium alginate-based nanofluid flow containing alumina nanoparticles over a bi-directional extending sheet using variable porous medium and slip conditions
  61. A comprehensive study of laser irradiated hydrothermally synthesized 2D layered heterostructure V2O5(1−x)MoS2(x) (X = 1–5%) nanocomposites for photocatalytic application
  62. Computational analysis of water-based silver, copper, and alumina hybrid nanoparticles over a stretchable sheet embedded in a porous medium with thermophoretic particle deposition effects
  63. A deep dive into AI integration and advanced nanobiosensor technologies for enhanced bacterial infection monitoring
  64. Effects of normal strain on pyramidal I and II 〈c + a〉 screw dislocation mobility and structure in single-crystal magnesium
  65. Computational study of cross-flow in entropy-optimized nanofluids
  66. Significance of nanoparticle aggregation for thermal transport over magnetized sensor surface
  67. A green and facile synthesis route of nanosize cupric oxide at room temperature
  68. Effect of annealing time on bending performance and microstructure of C19400 alloy strip
  69. Chitosan-based Mupirocin and Alkanna tinctoria extract nanoparticles for the management of burn wound: In vitro and in vivo characterization
  70. Electrospinning of MNZ/PLGA/SF nanofibers for periodontitis
  71. Photocatalytic degradation of methylene blue by Nd-doped titanium dioxide thin films
  72. Shell-core-structured electrospinning film with sequential anti-inflammatory and pro-neurogenic effects for peripheral nerve repairment
  73. Flow and heat transfer insights into a chemically reactive micropolar Williamson ternary hybrid nanofluid with cross-diffusion theory
  74. One-pot fabrication of open-spherical shapes based on the decoration of copper sulfide/poly-O-amino benzenethiol on copper oxide as a promising photocathode for hydrogen generation from the natural source of Red Sea water
  75. A penta-hybrid approach for modeling the nanofluid flow in a spatially dependent magnetic field
  76. Advancing sustainable agriculture: Metal-doped urea–hydroxyapatite hybrid nanofertilizer for agro-industry
  77. Utilizing Ziziphus spina-christi for eco-friendly synthesis of silver nanoparticles: Antimicrobial activity and promising application in wound healing
  78. Plant-mediated synthesis, characterization, and evaluation of a copper oxide/silicon dioxide nanocomposite by an antimicrobial study
  79. Effects of PVA fibers and nano-SiO2 on rheological properties of geopolymer mortar
  80. Investigating silver and alumina nanoparticles’ impact on fluid behavior over porous stretching surface
  81. Potential pharmaceutical applications and molecular docking study for green fabricated ZnO nanoparticles mediated Raphanus sativus: In vitro and in vivo study
  82. Effect of temperature and nanoparticle size on the interfacial layer thickness of TiO2–water nanofluids using molecular dynamics
  83. Characteristics of induced magnetic field on the time-dependent MHD nanofluid flow through parallel plates
  84. Flexural and vibration behaviours of novel covered CFRP composite joints with an MWCNT-modified adhesive
  85. Experimental research on mechanically and thermally activation of nano-kaolin to improve the properties of ultra-high-performance fiber-reinforced concrete
  86. Analysis of variable fluid properties for three-dimensional flow of ternary hybrid nanofluid on a stretching sheet with MHD effects
  87. Biodegradability of corn starch films containing nanocellulose fiber and thymol
  88. Toxicity assessment of copper oxide nanoparticles: In vivo study
  89. Some measures to enhance the energy output performances of triboelectric nanogenerators
  90. Reinforcement of graphene nanoplatelets on water uptake and thermomechanical behaviour of epoxy adhesive subjected to water ageing conditions
  91. Optimization of preparation parameters and testing verification of carbon nanotube suspensions used in concrete
  92. Max-phase Ti3SiC2 and diverse nanoparticle reinforcements for enhancement of the mechanical, dynamic, and microstructural properties of AA5083 aluminum alloy via FSP
  93. Advancing drug delivery: Neural network perspectives on nanoparticle-mediated treatments for cancerous tissues
  94. PEG-PLGA core–shell nanoparticles for the controlled delivery of picoplatin–hydroxypropyl β-cyclodextrin inclusion complex in triple-negative breast cancer: In vitro and in vivo study
  95. Conduction transportation from graphene to an insulative polymer medium: A novel approach for the conductivity of nanocomposites
  96. Review Articles
  97. Developments of terahertz metasurface biosensors: A literature review
  98. Overview of amorphous carbon memristor device, modeling, and applications for neuromorphic computing
  99. Advances in the synthesis of gold nanoclusters (AuNCs) of proteins extracted from nature
  100. A review of ternary polymer nanocomposites containing clay and calcium carbonate and their biomedical applications
  101. Recent advancements in polyoxometalate-functionalized fiber materials: A review
  102. Special contribution of atomic force microscopy in cell death research
  103. A comprehensive review of oral chitosan drug delivery systems: Applications for oral insulin delivery
  104. Cellular senescence and nanoparticle-based therapies: Current developments and perspectives
  105. Cyclodextrins-block copolymer drug delivery systems: From design and development to preclinical studies
  106. Micelle-based nanoparticles with stimuli-responsive properties for drug delivery
  107. Critical assessment of the thermal stability and degradation of chemically functionalized nanocellulose-based polymer nanocomposites
  108. Research progress in preparation technology of micro and nano titanium alloy powder
  109. Nanoformulations for lysozyme-based additives in animal feed: An alternative to fight antibiotic resistance spread
  110. Incorporation of organic photochromic molecules in mesoporous silica materials: Synthesis and applications
  111. A review on modeling of graphene and associated nanostructures reinforced concrete
  112. A review on strengthening mechanisms of carbon quantum dots-reinforced Cu-matrix nanocomposites
  113. Review on nanocellulose composites and CNFs assembled microfiber toward automotive applications
  114. Nanomaterial coating for layered lithium rich transition metal oxide cathode for lithium-ion battery
  115. Application of AgNPs in biomedicine: An overview and current trends
  116. Nanobiotechnology and microbial influence on cold adaptation in plants
  117. Hepatotoxicity of nanomaterials: From mechanism to therapeutic strategy
  118. Applications of micro-nanobubble and its influence on concrete properties: An in-depth review
  119. A comprehensive systematic literature review of ML in nanotechnology for sustainable development
  120. Exploiting the nanotechnological approaches for traditional Chinese medicine in childhood rhinitis: A review of future perspectives
  121. Twisto-photonics in two-dimensional materials: A comprehensive review
  122. Current advances of anticancer drugs based on solubilization technology
  123. Recent process of using nanoparticles in the T cell-based immunometabolic therapy
  124. Future prospects of gold nanoclusters in hydrogen storage systems and sustainable environmental treatment applications
  125. Preparation, types, and applications of one- and two-dimensional nanochannels and their transport properties for water and ions
  126. Microstructural, mechanical, and corrosion characteristics of Mg–Gd–x systems: A review of recent advancements
  127. Functionalized nanostructures and targeted delivery systems with a focus on plant-derived natural agents for COVID-19 therapy: A review and outlook
  128. Mapping evolution and trends of cell membrane-coated nanoparticles: A bibliometric analysis and scoping review
  129. Nanoparticles and their application in the diagnosis of hepatocellular carcinoma
  130. In situ growth of carbon nanotubes on fly ash substrates
  131. Structural performance of boards through nanoparticle reinforcement: An advance review
  132. Reinforcing mechanisms review of the graphene oxide on cement composites
  133. Seed regeneration aided by nanomaterials in a climate change scenario: A comprehensive review
  134. Surface-engineered quantum dot nanocomposites for neurodegenerative disorder remediation and avenue for neuroimaging
  135. Graphitic carbon nitride hybrid thin films for energy conversion: A mini-review on defect activation with different materials
  136. Nanoparticles and the treatment of hepatocellular carcinoma
  137. Special Issue on Advanced Nanomaterials and Composites for Energy Conversion and Storage - Part II
  138. Highly safe lithium vanadium oxide anode for fast-charging dendrite-free lithium-ion batteries
  139. Recent progress in nanomaterials of battery energy storage: A patent landscape analysis, technology updates, and future prospects
  140. Special Issue on Advanced Nanomaterials for Carbon Capture, Environment and Utilization for Energy Sustainability - Part II
  141. Calcium-, magnesium-, and yttrium-doped lithium nickel phosphate nanomaterials as high-performance catalysts for electrochemical water oxidation reaction
  142. Low alkaline vegetation concrete with silica fume and nano-fly ash composites to improve the planting properties and soil ecology
  143. Mesoporous silica-grafted deep eutectic solvent-based mixed matrix membranes for wastewater treatment: Synthesis and emerging pollutant removal performance
  144. Electrochemically prepared ultrathin two-dimensional graphitic nanosheets as cathodes for advanced Zn-based energy storage devices
  145. Enhanced catalytic degradation of amoxicillin by phyto-mediated synthesised ZnO NPs and ZnO-rGO hybrid nanocomposite: Assessment of antioxidant activity, adsorption, and thermodynamic analysis
  146. Incorporating GO in PI matrix to advance nanocomposite coating: An enhancing strategy to prevent corrosion
  147. Synthesis, characterization, thermal stability, and application of microporous hyper cross-linked polyphosphazenes with naphthylamine group for CO2 uptake
  148. Engineering in ceramic albite morphology by the addition of additives: Carbon nanotubes and graphene oxide for energy applications
  149. Nanoscale synergy: Optimizing energy storage with SnO2 quantum dots on ZnO hexagonal prisms for advanced supercapacitors
  150. Aging assessment of silicone rubber materials under corona discharge accompanied by humidity and UV radiation
  151. Tuning structural and electrical properties of Co-precipitated and Cu-incorporated nickel ferrite for energy applications
  152. Sodium alginate-supported AgSr nanoparticles for catalytic degradation of malachite green and methyl orange in aqueous medium
  153. An environmentally greener and reusability approach for bioenergy production using Mallotus philippensis (Kamala) seed oil feedstock via phytonanotechnology
  154. Micro-/nano-alumina trihydrate and -magnesium hydroxide fillers in RTV-SR composites under electrical and environmental stresses
  155. Mechanism exploration of ion-implanted epoxy on surface trap distribution: An approach to augment the vacuum flashover voltages
  156. Nanoscale engineering of semiconductor photocatalysts boosting charge separation for solar-driven H2 production: Recent advances and future perspective
  157. Excellent catalytic performance over reduced graphene-boosted novel nanoparticles for oxidative desulfurization of fuel oil
  158. Special Issue on Advances in Nanotechnology for Agriculture
  159. Deciphering the synergistic potential of mycogenic zinc oxide nanoparticles and bio-slurry formulation on phenology and physiology of Vigna radiata
  160. Nanomaterials: Cross-disciplinary applications in ornamental plants
  161. Special Issue on Catechol Based Nano and Microstructures
  162. Polydopamine films: Versatile but interface-dependent coatings
  163. In vitro anticancer activity of melanin-like nanoparticles for multimodal therapy of glioblastoma
  164. Poly-3,4-dihydroxybenzylidenhydrazine, a different analogue of polydopamine
  165. Chirality and self-assembly of structures derived from optically active 1,2-diaminocyclohexane and catecholamines
  166. Advancing resource sustainability with green photothermal materials: Insights from organic waste-derived and bioderived sources
  167. Bioinspired neuromelanin-like Pt(iv) polymeric nanoparticles for cancer treatment
  168. Special Issue on Implementing Nanotechnology for Smart Healthcare System
  169. Intelligent explainable optical sensing on Internet of nanorobots for disease detection
  170. Special Issue on Green Mono, Bi and Tri Metallic Nanoparticles for Biological and Environmental Applications
  171. Tracking success of interaction of green-synthesized Carbopol nanoemulgel (neomycin-decorated Ag/ZnO nanocomposite) with wound-based MDR bacteria
  172. Green synthesis of copper oxide nanoparticles using genus Inula and evaluation of biological therapeutics and environmental applications
  173. Biogenic fabrication and multifunctional therapeutic applications of silver nanoparticles synthesized from rose petal extract
  174. Metal oxides on the frontlines: Antimicrobial activity in plant-derived biometallic nanoparticles
  175. Controlling pore size during the synthesis of hydroxyapatite nanoparticles using CTAB by the sol–gel hydrothermal method and their biological activities
  176. Special Issue on State-of-Art Advanced Nanotechnology for Healthcare
  177. Applications of nanomedicine-integrated phototherapeutic agents in cancer theranostics: A comprehensive review of the current state of research
  178. Smart bionanomaterials for treatment and diagnosis of inflammatory bowel disease
  179. Beyond conventional therapy: Synthesis of multifunctional nanoparticles for rheumatoid arthritis therapy
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