Evaluation of the Efficiency of Detection and Capture of Manganese in Aqueous Solutions of FeCeOx Nanocomposites Doped with Nb2O5

The main purpose of this work is to study the effectiveness of using FeCeOx nanocomposites doped with Nb2O5 for the purification of aqueous solutions from manganese. X-ray diffraction, energy–dispersive analysis, scanning electron microscopy, vibrational magnetic spectroscopy, and mössbauer spectroscopy were used as research methods. It is shown that an increase in the dopant concentration leads to the transformation of the shape of nanoparticles from spherical to cubic and rhombic, followed by an increase in the size of the nanoparticles. The spherical shape of the nanoparticles is characteristic of a structure consisting of a mixture of two phases of hematite (Fe2O3) and cerium oxide CeO2. The cubic shape of nanoparticles is typical for spinel-type FeNbO4 structures, the phase contribution of which increases with increasing dopant concentration. It is shown that doping leads not only to a decrease in the concentration of manganese in model solutions, but also to an increase in the efficiency of adsorption from 11% to 75%.


Introduction
In recent years, special attention has been paid to nanocomposites based on metal oxides or ferrites, interest in which is due to the high potential for their use as catalysts, the basis for carriers of drugs, sensors and adsorbents of pollutants, and waste water treatment [1][2][3][4][5]. The wide range of their application is based on the possibility of obtaining nanostructured composites with large specific surface area, functional groups, and resistance to degradation [6,7]. Magnetic characteristics such as coercivity and saturation magnetization in turn allow the use of nanoparticles for purification of aqueous media by adsorption of contaminants on its surface and subsequent removal from solution by magnetic separation [8][9][10].
Among the variety of metal oxide nanocomposites and nanoparticles FeCeO x structures of the type have great potential in photocatalysis, biomedicine, purification of aqueous media, etc. [7][8][9][10][11][12]. Methods for preparing FeCeO x nanostructures are quite numerous, and in most of them

Experimental Part
The synthesis of nanocomposites was carried out in two stages, including the chemical deposition of FeCeO x (which is a mixture of two phases Fe 2 O 3 and CeO 2 ) [26] and subsequent mechanochemical mixing of amorphous-like FeCeO x nanoparticles with Nb 2 O 5 nanoparticles in the set stoichiometric proportions and thermal annealing in the air atmosphere at a temperature of 1000 • C within 8 h.
The samples were cooled down together with a muffle furnace (Naberthetm, Bremen, Germany) for 24 h. The choice of the annealing temperature is due to phase transformations in FeCeO х nanoparticles with the formation of two stable phases Fe 2 O 3 and CeO 2 . Earlier in [26], we examined in detail the phase transformations of FeCeO х nanoparticles as a result of thermal annealing in the temperature range from 400 to 800 • C, according to which, when the annealing temperature is increased above 600 • C, the structure of nanoparticles is a mixture of two phases Fe 2 O 3 and CeO 2 . In this case, an increase in temperature leads to an increase in the degree of structural ordering and a decrease in distortions and deformations of the crystal lattice. However, experimental work with an increase in the annealing temperature above 1000 • C led to the formation of large agglomerates of micron-sized particles that are not suitable for research.
The study of changes in the shape and size of nanoparticles as a result of changes in the concentration of the dopant was carried out by analyzing images obtained using a scanning electron microscope TM3030 (Hitachi Ltd., Chiyoda, Tokyo, Japan). The study of the elemental composition and its change were carried out using the method of energy dispersive analysis performed on the attachment Bruker XFlash MIN SVE microanalysis system at voltage of 15 kV.
The phase composition and the dynamics of its change as a result of doping were determined on the basis of the obtained diffractograms recorded on a D8 Advance ECO powder diffractometer (Bruker), in the Bragg-Brentano geometry in the angle range 2θ = 20-80 • with a step of 0.03 • , radiation Cu-Kλ = 1.54 Å.
The determination of magnetic characteristics was carried out using the vibration magnetic spectroscopy method performed on the "Liquid Helium Free High Field Measurement System", "Cryogenic LTD".
The study of ultrafine magnetic parameters was carried out using the method of Mössbauer spectroscopy on the MS1104Em Mössbauer spectrometer (Ritverc, Chernogolovka, Russia) with a 57 Co nuclei in the Rh matrix source. The calibration of the spectra obtained at room temperature was carried out using α-Fe absorber (Ritverc, Chernogolovka, Russia).
The study of the prospects of using the synthesized nanoparticles before and after doping as a basis for the purification of aqueous media from manganese by adsorption on the surface of nanoparticles and subsequent filtration was carried out using model aqueous solutions with a diluted manganese concentration of 22 mg/dm 3 . During the experiment, the solution was stirred to avoid the formation of a precipitate at the bottom of the beaker. Determination of the concentration of manganese before and after adsorption was carried out by determining the optical density in the wavelength range of 440-460 nm using the analyzer "Fluorat-02". The concentration of nanoparticles was 0.001 g, the adsorption time was 5 h. After the end of the time, the nanoparticles were captured by the magnet and removed from the model medium. Figure 1 shows images obtained using the method of scanning electron microscopy of synthesized nanoparticles before and after modification by doping. In the initial state, FeCeO 3 nanoparticles are spherical particles, the average size of which, according to the distribution diagram (see Figure 2a), varies from 110-120 nm.

Results and Discussion
Sensors 2020, 20, x 3 of 16 nanoparticles and subsequent filtration was carried out using model aqueous solutions with a diluted manganese concentration of 22 mg/dm 3 . During the experiment, the solution was stirred to avoid the formation of a precipitate at the bottom of the beaker. Determination of the concentration of manganese before and after adsorption was carried out by determining the optical density in the wavelength range of 440-460 nm using the analyzer "Fluorat-02". The concentration of nanoparticles was 0.001 g, the adsorption time was 5 h. After the end of the time, the nanoparticles were captured by the magnet and removed from the model medium. Figure 1 shows images obtained using the method of scanning electron microscopy of synthesized nanoparticles before and after modification by doping. In the initial state, FeCeO3 nanoparticles are spherical particles, the average size of which, according to the distribution diagram (see Figure 2a), varies from 110-120 nm. Doping of Nb2O5 with increasing concentration leads to changes not only in the size of nanoparticles, but also in the shape. A schematic representation of the resizing is shown in Figure 3. Initially, spherical nanoparticles undergo transformation in several stages, depending on the concentration of the dopant. In the case when the concentration is 0.1-0.2 of the total mass of mixed nanoparticles, spherical nanoparticles first lose their shape due to fouling by growths and cubic or diamond-shaped inclusions, which is also reflected in changes in the size of nanoparticles (see Figure  2b,c) by the appearance of a second maximum in the region 60-70 nm. An increase in the concentration of the dopant to 0.3 leads to a complete transformation of nanoparticles from a spherical to a cubic or rhomboid shape, accompanied by an increase in the size of nanoparticles to 150-170 nm (see Figure 2d).  Doping of Nb 2 O 5 with increasing concentration leads to changes not only in the size of nanoparticles, but also in the shape. A schematic representation of the resizing is shown in Figure 3. Initially, spherical nanoparticles undergo transformation in several stages, depending on the concentration of the dopant. In the case when the concentration is 0.1-0.2 of the total mass of mixed nanoparticles, spherical nanoparticles first lose their shape due to fouling by growths and cubic or diamond-shaped inclusions, which is also reflected in changes in the size of nanoparticles (see Figure  2b,c) by the appearance of a second maximum in the region 60-70 nm. An increase in the concentration of the dopant to 0.3 leads to a complete transformation of nanoparticles from a spherical to a cubic or rhomboid shape, accompanied by an increase in the size of nanoparticles to 150-170 nm (see Figure 2d).  Initially, spherical nanoparticles undergo transformation in several stages, depending on the concentration of the dopant. In the case when the concentration is 0.1-0.2 of the total mass of mixed nanoparticles, spherical nanoparticles first lose their shape due to fouling by growths and cubic or diamond-shaped inclusions, which is also reflected in changes in the size of nanoparticles (see Figure 2b,c) by the appearance of a second maximum in the region 60-70 nm. An increase in the concentration of the dopant to 0.3 leads to a complete transformation of nanoparticles from a spherical to a cubic or rhomboid shape, accompanied by an increase in the size of nanoparticles to 150-170 nm (see Figure 2d).

Results and Discussion
The Table 1 shows the elemental analysis data of the studied nanoparticles depending on the concentration of the dopant, as well as the specific surface area and the ratio of spherical and cubic nanoparticles. Table 1. Elemental analysis data, specific surface area, and particle type ratio. As can be seen from the presented data, an increase in the concentration of the dopant Nb 2 O 5 leads to the displacement of cerium atoms from the structure, while the iron content remains practically unchanged. Moreover, a change in the shape and size of nanoparticles leads to an increase in the specific surface area. However, for the case when the concentration of the dopant Nb 2 O 5 was 0.3 of the total mass, which is characterized by the transformation of nanoparticles from a spherical to a cubic shape, a decrease in the specific surface area is observed. Furthermore, a change in the concentration of the dopant Nb 2 O 5 leads to a change in the ratio of the types of particles with an almost complete predominance of the cubic and rhombic forms at a concentration of the dopant Nb 2 O 5 of 0.3 of the total mass.
The assessment of the phase composition of the studied nanoparticles depending on the concentration of the dopant Nb 2 O 5 is presented in Figure 4 (X-ray diffraction data) and Figure 5 (phase composition data). The general view of the diffraction patterns obtained using the shooting method in the Bragg-Brentano geometry indicates the polycrystallinity of the synthesized nanoparticles, as well as the presence of structural distortions arising in the process of grinding and subsequent thermal annealing.
Sensors 2020, 20, x 5 of 16 The Table 1 shows the elemental analysis data of the studied nanoparticles depending on the concentration of the dopant, as well as the specific surface area and the ratio of spherical and cubic nanoparticles. Table 1. Elemental analysis data, specific surface area, and particle type ratio. As can be seen from the presented data, an increase in the concentration of the dopant Nb2O5 leads to the displacement of cerium atoms from the structure, while the iron content remains practically unchanged. Moreover, a change in the shape and size of nanoparticles leads to an increase in the specific surface area. However, for the case when the concentration of the dopant Nb2O5 was 0.3 of the total mass, which is characterized by the transformation of nanoparticles from a spherical to a cubic shape, a decrease in the specific surface area is observed. Furthermore, a change in the concentration of the dopant Nb2O5 leads to a change in the ratio of the types of particles with an almost complete predominance of the cubic and rhombic forms at a concentration of the dopant Nb2O5 of 0.3 of the total mass.
The assessment of the phase composition of the studied nanoparticles depending on the concentration of the dopant Nb2O5 is presented in Figure 4 (X-ray diffraction data) and Figure 5 (phase composition data). The general view of the diffraction patterns obtained using the shooting method in the Bragg-Brentano geometry indicates the polycrystallinity of the synthesized nanoparticles, as well as the presence of structural distortions arising in the process of grinding and subsequent thermal annealing.  The different shapes of diffraction reflections for the initial sample indicate the presence in the structure of two phases characteristic of hematite (Fe 2 O 3 ) and cerium oxide CeO 2 , the phase ratio of which is approximately 1:2. In the case of doped nanoparticles, a change in the diffraction patterns is observed associated with the appearance of new additional peaks at 2θ = 24.2 • , 25.7 • , 28.1 • , 30.2 • , 31.8 • , and 32.9 • , characteristic of the monoclinic phase of FeNbO 4 -spinel type, whose contribution increases with increasing concentration dopant. In this case, the peaks characteristic of the Fe 2 O 3 and CeO 2 phases are also present in the diffractograms; however, their intensities decrease with an increase in the dopant concentration. The appearance of a new FeNbO 4 phase in the structure of nanoparticles indicates a phase transformation that occurs during grinding and subsequent annealing. The diagrams of the phase ratios in the composition of nanoparticles presented in Figure 5 were obtained by full-profile analysis of X-ray diffractograms with the subsequent calculation of the contributions according to formula (1) [27]: I phase is the value of the integral intensity of the main phase, I admixture is the value of the integral intensities of impurity phases, the structure factor is R = 1.45.
Sensors 2020, 20, x 6 of 16 The different shapes of diffraction reflections for the initial sample indicate the presence in the structure of two phases characteristic of hematite (Fe2O3) and cerium oxide CeO2, the phase ratio of which is approximately 1:2. In the case of doped nanoparticles, a change in the diffraction patterns is observed associated with the appearance of new additional peaks at 2θ = 24.2°, 25.7°, 28.1°, 30.2°, 31.8°, and 32.9°, characteristic of the monoclinic phase of FeNbO4-spinel type, whose contribution increases with increasing concentration dopant. In this case, the peaks characteristic of the Fe2O3 and CeO2 phases are also present in the diffractograms; however, their intensities decrease with an increase in the dopant concentration. The appearance of a new FeNbO4 phase in the structure of nanoparticles indicates a phase transformation that occurs during grinding and subsequent annealing. The diagrams of the phase ratios in the composition of nanoparticles presented in Figure  5 were obtained by full-profile analysis of X-ray diffractograms with the subsequent calculation of the contributions according to formula (1) [27]: Iphase is the value of the integral intensity of the main phase, Iadmixture is the value of the integral intensities of impurity phases, the structure factor is R = (c) (d) According to the data presented in the diffraction patterns, an increase in the concentration of the dopant Nb2O5 leads to the displacement of the CeO2 phase from the structure of nanoparticles, as well as to the dominance of the FeNbO4 phase. In this case, a change in the phase composition leads to a change in the density of nanoparticles, the data of which are shown in Figure 6. According to the data presented in the diffraction patterns, an increase in the concentration of the dopant Nb 2 O 5 leads to the displacement of the CeO 2 phase from the structure of nanoparticles, as well as to the dominance of the FeNbO 4 phase. In this case, a change in the phase composition leads to a change in the density of nanoparticles, the data of which are shown in Figure 6. The magnetic characteristics of nanoparticles depending on the concentration of the dopant were studied using a vibrating magnetometer, hysteresis loops are shown in Figure 7, the results of calculating the magnetic characteristics are presented in Table 2. Magnetization (emu/g)  The magnetic characteristics of nanoparticles depending on the concentration of the dopant were studied using a vibrating magnetometer, hysteresis loops are shown in Figure 7, the results of calculating the magnetic characteristics are presented in Table 2.  The magnetic characteristics of nanoparticles depending on the concentration of the dopant were studied using a vibrating magnetometer, hysteresis loops are shown in Figure 7, the results of calculating the magnetic characteristics are presented in Table 2.     [27][28][29], which is associated with the particle size of iron oxide and its fraction in the composites. With sizes up to tens of nanometers, particles have superparamagnetic characteristics, with large sizes-ferromagnetic properties. The samples in question have an average size of 120 nm and have ferromagnetic properties, and low values of specific parameters are explained by the high content of non-magnetic phase in the composite.
When Nb 2 O 5 is introduced into the reaction mixture and the FeNbO 4 phase is formed in the structure of nanoparticles, there is a sharp change in the magnetic parameters, the connectivity increases 13 times for 0.9FeCeO x + 0.1Nb 2 O 5 nanoparticles and 10 times for 0.8FeCeO x + 0.2Nb 2 O 5 nanoparticles, the quadraticity of the hysteresis loops changes. The observed change is associated with surface magnetic effects occurring on FeCeO x particles, apparently, by the pinning of magnetic moments due to the formation of a new phase. However, a significant change in the phase composition in the 0.7FeCeO x + 0.3Nb 2 O 5 nanoparticles sample and the formation of a new shape of structures leads to a weakening of the surface effects and a halving of the coercivity.
The estimation of the hyperfine magnetic parameters of the synthesized nanoparticles, as well as the effect of doping on the degree of magnetic disordering, was carried out by analyzing the Mössbauer spectra obtained at room temperature. The general view of the spectrum of nanoparticles in the initial state is characterized by the presence of two sextets of ultrafine magnetic fields of 515-516 kOe, which are characteristic of two types of ferromagnetic iron atoms (see Figure 8). The values of the hyperfine fields and also isomeric shifts for the initial nanoparticles are characteristic of structures such as hematite Fe 2 O 3 with a partially disordered structure. Disordering and deviation of the hyperfine fields from the reference values of hematite is due to the presence of the CeO 2 phase in the structure of nanoparticles. Additionally, the influence of the CeO 2 phase on the degree of magnetic and structural ordering is evidenced by the ratio of the contributions of the partial spectra of two sextets 2.11:0.89, which is characteristic of the violation of stoichiometry at various levels of population in the A-and B-sublattices.   1 Hc, Oe-coercivity, 2 Mr, emu/g-remanent magnetization, 3 Ms, emu/g-saturation magnetization, 4 Mr/Ms-squareness.
In the initial state, nanoparticles have a significant coercivity value Hc = 200, Oe and small values of specific magnetic parameters Mr = 0.0375, emu/g, Ms = 0.26, emu/g.
The literature provides various values of magnetic parameters of the composite FeCeOx [27][28][29], which is associated with the particle size of iron oxide and its fraction in the composites. With sizes up to tens of nanometers, particles have superparamagnetic characteristics, with large sizes-ferromagnetic properties. The samples in question have an average size of 120 nm and have ferromagnetic properties, and low values of specific parameters are explained by the high content of non-magnetic phase in the composite.
When Nb2O5 is introduced into the reaction mixture and the FeNbO4 phase is formed in the structure of nanoparticles, there is a sharp change in the magnetic parameters, the connectivity increases 13 times for 0.9FeCeOx + 0.1Nb2O5 nanoparticles and 10 times for 0.8FeCeOx + 0.2Nb2O5 nanoparticles, the quadraticity of the hysteresis loops changes. The observed change is associated with surface magnetic effects occurring on FeCeOx particles, apparently, by the pinning of magnetic moments due to the formation of a new phase. However, a significant change in the phase composition in the 0.7FeCeOx + 0.3Nb2O5 nanoparticles sample and the formation of a new shape of structures leads to a weakening of the surface effects and a halving of the coercivity.
The estimation of the hyperfine magnetic parameters of the synthesized nanoparticles, as well as the effect of doping on the degree of magnetic disordering, was carried out by analyzing the Mössbauer spectra obtained at room temperature. The general view of the spectrum of nanoparticles in the initial state is characterized by the presence of two sextets of ultrafine magnetic fields of 515-516 kOe, which are characteristic of two types of ferromagnetic iron atoms (see Figure 8). The values of the hyperfine fields and also isomeric shifts for the initial nanoparticles are characteristic of structures such as hematite Fe2O3 with a partially disordered structure. Disordering and deviation of the hyperfine fields from the reference values of hematite is due to the presence of the CeO2 phase in the structure of nanoparticles. Additionally, the influence of the CeO2 phase on the degree of magnetic and structural ordering is evidenced by the ratio of the contributions of the partial spectra of two sextets 2.11:0.89, which is characteristic of the violation of stoichiometry at various levels of population in the A-and B-sublattices.   For microparticles doped with Nb2O5 the emergence of a doublet and also decrease in the intensities of two sextets with the subsequent complete dominance of a doublet in the structure of the spectrum of 0.7FeCeOx + 0.3 Nb2O5 nanoparticles is observed. The appearance of a quadrupole paramagnetic doublet and the subsequent increase in its contribution is due to the doping effect and partial replacement of iron atoms with niobium with the subsequent formation of a spinel structure. At the same time, the decrease in the value of ultra-thin magnetic fields in the case of an increase in the concentration of dopant Nb2O5 may be due to the presence of a phase FeNbO4 in the structure, which is characterized by the spinel structure. Figure 10 shows the data on changes in the cyclic current-voltage characteristics of the studied nanoparticles depending on the concentration of the dopant. For the initial nanoparticles, the nature of the change in the cyclic volt-amperogram has a nonlinear non-ohmic character, characterized by a region from 0.2 to 1.5 V with a sharp increase in conductivity, characteristic of the quadratic     For microparticles doped with Nb2O5 the emergence of a doublet and also decrease in the intensities of two sextets with the subsequent complete dominance of a doublet in the structure of the spectrum of 0.7FeCeOx + 0.3 Nb2O5 nanoparticles is observed. The appearance of a quadrupole paramagnetic doublet and the subsequent increase in its contribution is due to the doping effect and partial replacement of iron atoms with niobium with the subsequent formation of a spinel structure. At the same time, the decrease in the value of ultra-thin magnetic fields in the case of an increase in the concentration of dopant Nb2O5 may be due to the presence of a phase FeNbO4 in the structure, which is characterized by the spinel structure. Figure 10 shows the data on changes in the cyclic current-voltage characteristics of the studied nanoparticles depending on the concentration of the dopant. For the initial nanoparticles, the nature of the change in the cyclic volt-amperogram has a nonlinear non-ohmic character, characterized by a region from 0.2 to 1.5 V with a sharp increase in conductivity, characteristic of the quadratic For microparticles doped with Nb 2 O 5 the emergence of a doublet and also decrease in the intensities of two sextets with the subsequent complete dominance of a doublet in the structure of the spectrum of 0.7FeCeO x + 0.3 Nb 2 O 5 nanoparticles is observed. The appearance of a quadrupole paramagnetic doublet and the subsequent increase in its contribution is due to the doping effect and partial replacement of iron atoms with niobium with the subsequent formation of a spinel structure. At the same time, the decrease in the value of ultra-thin magnetic fields in the case of an increase in the concentration of dopant Nb 2 O 5 may be due to the presence of a phase FeNbO 4 in the structure, which is characterized by the spinel structure. Figure 10 shows the data on changes in the cyclic current-voltage characteristics of the studied nanoparticles depending on the concentration of the dopant. For the initial nanoparticles, the nature of the change in the cyclic volt-amperogram has a nonlinear non-ohmic character, characterized by a region from 0.2 to 1.5 V with a sharp increase in conductivity, characteristic of the quadratic dependence of the change in current strength on the applied voltage, and subsequent smooth change in current strength depending on voltage. Furthermore, the presence of an abrupt behavior of a change in the current-voltage characteristic can be due to the presence of two phases in the structure, which create additional obstacles to the ballistic nature of charge transfer.
dependence of the change in current strength on the applied voltage, and subsequent smooth change in current strength depending on voltage. Furthermore, the presence of an abrupt behavior of a change in the current-voltage characteristic can be due to the presence of two phases in the structure, which create additional obstacles to the ballistic nature of charge transfer. For doped nanoparticles, the character of the change in current-voltage characteristics is close to ohmic, without the obvious presence of regions with a quadratic dependence of the change in I on V. In this case, the formation of the FeNbO4 phase at low concentrations leads to a sharp increase in the resistivity of nanoparticles (see Figure 11). However, the dominance of the FeNbO4 phase, as well as transformation processes in the shape of nanoparticles, lead to structure ordering and a decrease in the resistance value. For doped nanoparticles, the character of the change in current-voltage characteristics is close to ohmic, without the obvious presence of regions with a quadratic dependence of the change in I on V. In this case, the formation of the FeNbO 4 phase at low concentrations leads to a sharp increase in the resistivity of nanoparticles (see Figure 11). However, the dominance of the FeNbO 4 phase, as well as transformation processes in the shape of nanoparticles, lead to structure ordering and a decrease in the resistance value.   According to the presented data, in the case of using the initial nanoparticles, the efficiency of reducing the concentration of manganese in the model solution after filtration was no more than 11%, while for doped nanoparticles, an increase in the concentration of the dopant leads to a sharp increase from 24% to 75% (see Figure 12b). An increase in the adsorption capacity of doped nanoparticles is due to a change in the morphological features of nanoparticles, as well as structural transformations, which more actively interact with the model solution and adsorb manganese on their surface, followed by its deposition on the surface of nanoparticles in the form of build-ups and small particles, which are clearly visible on SEM images nanoparticles after the filtration process (see Figure 13).    According to the presented data, in the case of using the initial nanoparticles, the efficiency of reducing the concentration of manganese in the model solution after filtration was no more than 11%, while for doped nanoparticles, an increase in the concentration of the dopant leads to a sharp increase from 24% to 75% (see Figure 12b). An increase in the adsorption capacity of doped nanoparticles is due to a change in the morphological features of nanoparticles, as well as structural transformations, which more actively interact with the model solution and adsorb manganese on their surface, followed by its deposition on the surface of nanoparticles in the form of build-ups and small particles, which are clearly visible on SEM images nanoparticles after the filtration process (see Figure 13). According to the presented data, in the case of using the initial nanoparticles, the efficiency of reducing the concentration of manganese in the model solution after filtration was no more than 11%, while for doped nanoparticles, an increase in the concentration of the dopant leads to a sharp increase from 24% to 75% (see Figure 12b). An increase in the adsorption capacity of doped nanoparticles is due to a change in the morphological features of nanoparticles, as well as structural transformations, which more actively interact with the model solution and adsorb manganese on their surface, followed by its deposition on the surface of nanoparticles in the form of build-ups and small particles, which are clearly visible on SEM images nanoparticles after the filtration process (see Figure 13). A direct confirmation of the fact that the formed small growths on the surface of nanoparticles are manganese are the data of the mapping results, which are presented in Figure 14, obtained from the 0.7FeCeOx + 0.3 Nb2O5 nanoparticles samples. A direct confirmation of the fact that the formed small growths on the surface of nanoparticles are manganese are the data of the mapping results, which are presented in Figure 14, obtained from the 0.7FeCeO x + 0.3 Nb 2 O 5 nanoparticles samples. Figure 15a shows data on changes in the elemental content of manganese on the surface of nanoparticles, which was determined using the method of energy dispersive analysis. According to the data obtained, for the initial nanoparticles, the content of adsorbed manganese on the surface is no more than 4-5 at %, while for doped nanoparticles this value ranges from 7% to 12% depending on the concentration of the dopant. A direct confirmation of the fact that the formed small growths on the surface of nanoparticles are manganese are the data of the mapping results, which are presented in Figure 14, obtained from the 0.7FeCeOx + 0.3 Nb2O5 nanoparticles samples.   Figure 15a shows data on changes in the elemental content of manganese on the surface of nanoparticles, which was determined using the method of energy dispersive analysis. According to the data obtained, for the initial nanoparticles, the content of adsorbed manganese on the surface is no more than 4-5 at %, while for doped nanoparticles this value ranges from 7% to 12% depending on the concentration of the dopant. An important feature of magnetic nanoparticles used for purification of aqueous media or photocatalytic decomposition reactions is the possibility of their complete extraction from solutions after filtration and a cycle of reactions using magnets. Figure 15b shows the data on the efficiency of trapping nanoparticles using magnets after 5 h of filtration, from which it can be seen that the percentage of trapping nanoparticles after filtration is 97-100% for modified nanoparticles, which indicates that the magnetic properties of nanoparticles are preserved after filtration. In this case, the degree of capture of 87% for the initial nanoparticles indicates a partial degradation of nanoparticles during the experiment. So, for example, in work [30] it was shown that after 24 h of staying in an aqueous solution of nanoparticles, their partial degradation is observed due to the formation of paramagnetic inclusions, which can reduce the collection efficiency. In this case, a long stay in the model solution leads to a decrease in the filtration efficiency due to the degradation of nanoparticles. However, in our case, the choice of a filtration time of five hours does not lead to any significant changes in the morphology of nanoparticles, as well as their degradation.   Figure 15a shows data on changes in the elemental content of manganese on the surface of nanoparticles, which was determined using the method of energy dispersive analysis. According to the data obtained, for the initial nanoparticles, the content of adsorbed manganese on the surface is no more than 4-5 at %, while for doped nanoparticles this value ranges from 7% to 12% depending on the concentration of the dopant. An important feature of magnetic nanoparticles used for purification of aqueous media or photocatalytic decomposition reactions is the possibility of their complete extraction from solutions after filtration and a cycle of reactions using magnets. Figure 15b shows the data on the efficiency of trapping nanoparticles using magnets after 5 h of filtration, from which it can be seen that the percentage of trapping nanoparticles after filtration is 97-100% for modified nanoparticles, which indicates that the magnetic properties of nanoparticles are preserved after filtration. In this case, the degree of capture of 87% for the initial nanoparticles indicates a partial degradation of nanoparticles during the experiment. So, for example, in work [30] it was shown that after 24 h of staying in an aqueous solution of nanoparticles, their partial degradation is observed due to the formation of paramagnetic inclusions, which can reduce the collection efficiency. In this case, a long stay in the model solution leads to a decrease in the filtration efficiency due to the degradation of nanoparticles. However, in our case, the choice of a filtration time of five hours does not lead to any significant changes in the morphology of nanoparticles, as well as their degradation. An important feature of magnetic nanoparticles used for purification of aqueous media or photocatalytic decomposition reactions is the possibility of their complete extraction from solutions after filtration and a cycle of reactions using magnets. Figure 15b shows the data on the efficiency of trapping nanoparticles using magnets after 5 h of filtration, from which it can be seen that the percentage of trapping nanoparticles after filtration is 97-100% for modified nanoparticles, which indicates that the magnetic properties of nanoparticles are preserved after filtration. In this case, the degree of capture of 87% for the initial nanoparticles indicates a partial degradation of nanoparticles during the experiment. So, for example, in work [30] it was shown that after 24 h of staying in an aqueous solution of nanoparticles, their partial degradation is observed due to the formation of paramagnetic inclusions, which can reduce the collection efficiency. In this case, a long stay in the model solution leads to a decrease in the filtration efficiency due to the degradation of nanoparticles. However, in our case, the choice of a filtration time of five hours does not lead to any significant changes in the morphology of nanoparticles, as well as their degradation.

Conclusions
The paper demonstrates the efficiency of using FeCeO x doping of Nb 2 O 5 nanoparticles in order not only to change the morphology and phase composition of nanoparticles, but also to increase the adsorption of manganese and increase the degree of purification. Resistance to degradation with an increase in the concentration of the dopant Nb 2 O 5 , as well as an increase in the purification efficiency, is due to the presence of a stable phase of the spinel type FeNbO 4 in the structure. The high degree of capture efficiency for modified nanoparticles indicates the possibility of their reuse.
Further experiments will be aimed at studying the influence of various factors, such as the acidity of the medium, the concentration of nanoparticles in the model solution on the degree of purification.