Mechanosynthesis, Structure and Photoluminescent Properties of the Pr 3+ Doped LiNbO 3 , LiNbO 3 :Mg, LiTaO 3 Nanopowders

: In the current work, nanocrystalline powders with different compositions, namely Li 0.98 Pr 0.02 NbO 3 , Li 0.93 Pr 0.02 Mg 0.05 NbO 3 and Li 0.98 Pr 0.02 TaO 3 were synthesized for the ﬁrst time using the method of high-energy ball milling of the starting materials (Li 2 CO 3 , Nb 2 O 5 , Ta 2 O 5 , MgO, Pr 6 O 11 ), followed by high-temperature annealing. XRD data analysis conﬁrmed the absence of parasitic phases in the obtained nanocrystalline compounds. The estimated particle sizes ranged from 20 to 80 nm. From the obtained nanopowders, ceramic samples were prepared using specially developed equipment, which allowed for pressing at elevated temperatures with a simultaneous application of a constant electric ﬁeld. The obtained photoluminescence spectra exhibit characteristic features of Pr 3+ ions in the crystal structure of LiNbO 3 and LiTaO 3 and are most efﬁciently excited by UV light. Samples pressed with an electric ﬁeld application show higher intensity of photoluminescence. Investigations of the temperature dependence of electrical conductivity of the Li 0.98 Pr 0.02 NbO 3 sample, pressed with the application of an electric ﬁeld, indicate that the conductivity mechanism is similar to that of LiNbO 3 single crystals and, at high temperatures, is attributed to the lithium conduction mechanism.


Introduction
Lithium niobate (LiNbO 3 , LN) and lithium tantalate (LiTaO 3 , LT) single crystals doped with Pr 3+ ions (LN:Pr, LT:Pr) have attracted the researcher's attention since the 1990s [1,2].The Pr 3+ -doping of LN and LT allows to create effective oxide phosphors that emit light in the red region of the spectrum [3].Further, the unique physical and chemical properties of LiNbO 3 crystals make it possible to produce multifunctional active elements for optoelectronic devices and sensors.In this context, recent years' results concerning piezoluminescence in LN:Pr and LT:Pr are of particular interest, for example, for creating pressure sensors [4,5].Further, doped nanomaterials can be used as nanoscale fillers in glasses, polymers and liquids to modify their optical, electrophysical or magnetic properties.One recent example of such an application is the creation of a relatively stable colloid of lithium niobate nanoparticles [6].Further, recent research on up-conversion luminescence of erbium and ytterbium-doped lithium niobate nanoparticles has shown temperature dependence that holds promise for applications in thermometry [7].Moreover, the luminescent properties of praseodymium in other ferroelectric niobates also attracted attention as promising sensor materials [8][9][10][11][12].The strong intensity of mechano-and photoluminescence was observed by authors [3] in congruent LN:Pr single crystals grown by Czochralski technique as well as in LN congruent crystals, co-doped with Pr and Mg.Further, the study of the mechanoluminescent and photoluminescent properties of LiNbO 3 :Pr and LiTaO 3 :Pr, prepared in form of micropowders using solid-phase synthesis from a mixture of the corresponding starting oxides and lithium carbonate was performed in [4].To the best of our knowledge, nanocrystalline powders of LiNbO 3 and LiTaO 3 doped with Pr ions have not yet been synthesized and studied.However, they may be of practical importance as luminescent materials.Further, the investigations of nanopowder properties are often performed for samples, which are pressed and prepared as ceramics.However, for materials that exhibit ferroelectric properties (LN and LT), questions arise: will the polarization of individual particles influence the pressing processes, and how might the properties of the material, particularly its luminescent properties, change if the pressing process is performed at elevated temperatures and with simultaneous application of an electric field?
This work is focused on the study of LiNbO 3 , LiNbO 3 :Mg and LiTaO 3 nanopowders doped with Pr 3+ ions, which were obtained with the mechanosynthesis technique (highenergy ball milling and subsequent high-temperature annealing).Ceramic samples were prepared using specially designed equipment for pressing at elevated temperatures with a simultaneous application of an electric field in order to investigate the crystal structure, photoluminescence and electrophysical properties of obtained LN:Pr, LN:Mg,Pr and LT:Pr ceramic samples.
Phase compositions of obtained nanocrystalline powders were studied with the XRD analysis using the modernized DRON-3M diffractometer (Lviv, Ukraine).
Experimental pressing equipment and process will be described below (Section 3.2).In the experiments, a laboratory press, which could provide a force of 10 tons, was used.
The temperature dependence of electrical conductivity was determined with impedance measurements in the frequency range from 1 Hz to 1 MHz.For this purpose, a phase impedance gain analyzer (Solartron 1260, Ametek Scientific Instruments, Hampshire, UK) was used.The measurements were performed on LN:Pr pressed pellet with thickness of 1.3 mm and diameter of 10 mm.Platinum electrodes (6 mm in diameter) were deposited on both sides of the sample using screen printing (print ink: Ferro Corporation, No. 6412 0410).Subsequently, the sample was annealed at 1000 • C for 30 min to ensure the electrodes adhesion.

Synthesis and XRD Analysis of Nanopowders
In our previous studies [13][14][15], the technological advantages were shown for obtaining lithium niobate and lithium tantalate nanopowders with a mechanosynthesis technique compared to the wet chemistry method-a smaller number of operations, no need to use hazardous chemicals or a protective gas environment, high pressures, etc.In the present study, the nanopowders with nominal compositions Li 0.98 Pr 0.02 NbO 3 (denoted as LN:Pr), Li 0.93 Mg 0.05 Pr 0.02 NbO 3 (LN:Mg,Pr), Li 0.98 Pr 0.02 TaO 3 (LT:Pr) were obtained with high-energy ball milling and subsequent annealing of the corresponding powders mixtures (Li 2 CO 3 , Nb 2 O 5 , Ta 2 O 5 , MgO, Pr 6 O 11 ) taken in mass ratios corresponding to stoichiometric compositions.
The masses of the starting components are presented in Table 1.The starting components were loaded into the mill chamber with a volume of 200 mL in an air environment.Zirconium dioxide balls with a diameter of 5 mm and a total weight of 91.5 g were used as working bodies.The ratio of the mass of balls to the mass of reagents was in the range of 8.0-8.4.The optimal modes, established in [13], were used for the milling process: the rotation speed was 600 rpm and the time of mechanical treatment for each composition was 15 h.There were three cycles of 5 h each with intermediate "loosening" of the partially compressed reaction mixture and removing gases (primarily CO 2 ).Within each cycle, a reverse was applied every 30 min.
Mechanical processing of reagents ensures the activation of the surface of the particles.Still, it does not lead to the final synthesis of the crystalline nanopowder of the desired composition.The XRD pattern of LiNbO 3 :Pr powder only after grinding is shown in Figure 1 as an example and compared to the reference XRD pattern of LN.The results indicate the formation of a mostly amorphous precursor, the partial formation of the lithium niobate perovskite phase, and the partial decomposition of lithium carbonate.Therefore, the next stage of preparation of LN:Pr, LT:Pr and LN:Mg,Pr nanopowders involves heat treatment of the precursors obtained after milling at 700 °C for 5 h.The heating rate was 300 °C/h, and cooling took place together with the furnace after its power was turned off.After the annealing procedure, the phase composition of the nanopowders Therefore, the next stage of preparation of LN:Pr, LT:Pr and LN:Mg,Pr nanopowders involves heat treatment of the precursors obtained after milling at 700 • C for 5 h.The heating rate was 300 • C/h, and cooling took place together with the furnace after its power was turned off.After the annealing procedure, the phase composition of the nanopowders was again studied, and the related XRD patterns are shown in Figure 2. The XRD analysis of the synthesized compounds indicates the absence of parasitic phases.
2, deg.Therefore, the next stage of preparation of LN:Pr, LT:Pr and LN:Mg,Pr nanop involves heat treatment of the precursors obtained after milling at 700 °C for heating rate was 300 °C/h, and cooling took place together with the furnace after it was turned off.After the annealing procedure, the phase composition of the nanop was again studied, and the related XRD patterns are shown in Figure 2. The XRD of the synthesized compounds indicates the absence of parasitic phases.The average grain size of crystallites, which were evaluated from dependences of the Bragg's maxima peak broadening, is about 20-80 nm.T external standard was used as a correction of instrumental broadening.

Samples Pressing
It is not always convenient to deal with the material in the nanopowder form practical use or for the study of physical properties.This, in particular, is re The average grain size of crystallites, which were evaluated from angular dependences of the Bragg's maxima peak broadening, is about 20-80 nm.The LaB 6 external standard was used as a correction of instrumental broadening.

Samples Pressing
It is not always convenient to deal with the material in the nanopowder form for the practical use or for the study of physical properties.This, in particular, is related to luminescence studies when it is advisable to perform measurements on the most compacted samples.
Therefore, one of the tasks of this work was to develop special equipment for pressing pellets from nanopowders and to obtain ceramic samples for measurements.
As follows from the above data, the tantalum-containing ceramic samples were obtained and studied only in [24,27,28].In addition, the nanopowder obtained by the sol-gel method was used as the starting material for pressing in only one work.The lithium niobate-based ceramics activated by rare earth ions Yb and Ho were also investigated.In most of the examined sources, polyvinyl alcohol was used during pressing for better particle agglomeration, which eventually burned out of the pressed samples during annealing at 500-700 • C. In different works, the values of applied pressures varied from 3 to 980 MPa.As a rule, the pressed samples were annealed at 900-1200 • C for 1-6 h in an oxidizing atmosphere (air or flowing oxygen).It should be noted that the tablet hot pressing with the simultaneous application of electric field along with the heating of the sample was not considered in the studied works [11,12,[16][17][18][19][20][21][22][23][24][25][26][27][28].However, such an approach could have a positive influence in the case of ferroelectric materials pressing.The high temperature and electric field can contribute to greater compactness of the samples and at least partial ordering of the polar particles.Therefore, equipment for pressing nanopowders in an external electric field with the possibility of simultaneous heating was designed and manufactured for this work.The scheme of equipment for pressing nanopowders is shown in Figure 3.
particle agglomeration, which eventually burned out of the pressed samples annealing at 500-700 °C.In different works, the values of applied pressures varied to 980 MPa.As a rule, the pressed samples were annealed at 900-1200 °C for 1-6 oxidizing atmosphere (air or flowing oxygen).
It should be noted that the tablet hot pressing with the simultaneous applic electric field along with the heating of the sample was not considered in the studied [11,12,[16][17][18][19][20][21][22][23][24][25][26][27][28].However, such an approach could have a positive influence in the ferroelectric materials pressing.The high temperature and electric field can contr greater compactness of the samples and at least partial ordering of the polar p Therefore, equipment for pressing nanopowders in an external electric field w possibility of simultaneous heating was designed and manufactured for this wo scheme of equipment for pressing nanopowders is shown in Figure 3.The developed equipment allows us to study the photoluminescent prope nanocrystalline LN:Pr and LT:Pr obtained by mechanosynthesis.Moreover, it prov opportunity to study the influence of the pressing conditions on ceramic samples an luminescent properties.For comparison purposes, the pressing was performed modes:  with simultaneous heating and application of an electric field;  without heating and without applying an electric field.
The first mode needs for the determination of optimal ratios between the p temperature and the applied voltage to the sample.This is due to the danger of el breakdown with increased pressure and temperature.A current limit was set for th voltage converter, which should not exceed 3 mA at a voltage of 1 kV.The voltage was applied to the samples in all the experiments.Therefore, it was investigated h electric current changes during heating at different pressures.
Since the amount of the obtained LN:Pr, LN:Mg,Pr, LT:Pr nanopowders was the pressing experiments were firstly performed on LN micropowder of stoichi The developed equipment allows us to study the photoluminescent properties of nanocrystalline LN:Pr and LT:Pr obtained by mechanosynthesis.Moreover, it provides an opportunity to study the influence of the pressing conditions on ceramic samples and their luminescent properties.For comparison purposes, the pressing was performed in two modes:

•
with simultaneous heating and application of an electric field; • without heating and without applying an electric field.
The first mode needs for the determination of optimal ratios between the pressure, temperature and the applied voltage to the sample.This is due to the danger of electrical breakdown with increased pressure and temperature.A current limit was set for the highvoltage converter, which should not exceed 3 mA at a voltage of 1 kV.The voltage of 1 kV was applied to the samples in all the experiments.Therefore, it was investigated how the electric current changes during heating at different pressures.
Since the amount of the obtained LN:Pr, LN:Mg,Pr, LT:Pr nanopowders was limited, the pressing experiments were firstly performed on LN micropowder of stoichiometric composition as synthesized by the solid-phase reaction.This approach assumes that the general patterns of electric current dependence on pressure and temperature should be similar in the case of pressing nanopowder and micropowder.
The sample pressing with simultaneous heating and application of the electric field was carried out in the following sequence: 1.
powder loading in the amount of 0.4 g; 2.
start of the heating.
The heater was switched off after the current reached a value of 3 mA at a certain temperature.The sample was kept under the pressure and electric field for 15 min after reaching the specified temperature.After that, the heating of the furnace was turned off and cooled to room temperature along with the entire system.At room temperature, the high voltage was turned off, and the pressure was stopped.
The temperature dependencies of the current for different fixed pressures during the pressing of nanopowders are shown in Figure 4.
composition as synthesized by the solid-phase reaction.This approach assumes that the general patterns of electric current dependence on pressure and temperature should be similar in the case of pressing nanopowder and micropowder.
The sample pressing with simultaneous heating and application of the electric field was carried out in the following sequence: 1. powder loading in the amount of 0.4 g; 2. voltage application of 1 kV; 3. pressure application; 4. start of the heating.
The heater was switched off after the current reached a value of 3 mA at a certain temperature.The sample was kept under the pressure and electric field for 15 min after reaching the specified temperature.After that, the heating of the furnace was turned off and cooled to room temperature along with the entire system.At room temperature, the high voltage was turned off, and the pressure was stopped.
The temperature dependencies of the current for different fixed pressures during the pressing of nanopowders are shown in Figure 4.As can be seen from this figure, the current maxima are observed in the temperature range of 30-100 °C, regardless of the applied pressure.Such peaks were present in all of the pressing experiments of LN:Pr, LN:Mg,Pr, LT:Pr nanopowders with simultaneous heating and application of an electric field.Similar peaks were also observed during pressing of LN micropowders, which was initially performed for system testing purposes.It should be noted, however, that we did not conduct repeated experiments to study the temperature dependence of the current in already pressed samples.We also did not study the temperature dependence of the current in nanopowders without applying pressure.
Observed peaks in the range of 30-100 °C are attributed to the loss of the moisture adsorbed by the powders during storage.This assumption can be supported by the fact that the temperature position of the current peaks does not change with the applied pressure.Further, the electrical conductivity of nanopowders is activated at much lower temperatures with increasing pressure.Therefore, the energy position of the levels, if they were inherent in the compound itself and could participate in conductivity of lithium niobate or lithium tantalate, should also change under the influence of pressure, which is not observed.Moreover, the study of the temperature dependence of the electrical As can be seen from this figure, the current maxima are observed in the temperature range of 30-100 • C, regardless of the applied pressure.Such peaks were present in all of the pressing experiments of LN:Pr, LN:Mg,Pr, LT:Pr nanopowders with simultaneous heating and application of an electric field.Similar peaks were also observed during pressing of LN micropowders, which was initially performed for system testing purposes.It should be noted, however, that we did not conduct repeated experiments to study the temperature dependence of the current in already pressed samples.We also did not study the temperature dependence of the current in nanopowders without applying pressure.
Observed peaks in the range of 30-100 • C are attributed to the loss of the moisture adsorbed by the powders during storage.This assumption can be supported by the fact that the temperature position of the current peaks does not change with the applied pressure.Further, the electrical conductivity of nanopowders is activated at much lower temperatures with increasing pressure.Therefore, the energy position of the levels, if they were inherent in the compound itself and could participate in conductivity of lithium niobate or lithium tantalate, should also change under the influence of pressure, which is not observed.Moreover, the study of the temperature dependence of the electrical conductivity in single crystalline lithium niobate and lithium tantalate, performed in [29], did not reveal any extreme peculiarities in the temperature range of 290-450 K.
Further increase of the temperature leads to an exponential increase in the current, and the temperature, at which the current begins to increase, depends significantly on the applied pressure (see Figure 4).Based on the obtained results and the information given in Table 2, the following pressing conditions were chosen for LN:Pr, LN:Mg,Pr, LT:Pr nanopowders: An increase in the pressure above 190 MPa with simultaneous heating can cause an electrical breakdown of the pressed sample.Therefore, the proposed choice can be considered optimal for the configuration used in our study.
As an example, the temperature dependence of the current in the LN:Pr sample is presented in Figure 5.
conductivity in single crystalline lithium niobate and lithium tantalate, performed in [29], did not reveal any extreme peculiarities in the temperature range of 290-450 K.
Further increase of the temperature leads to an exponential increase in the current, and the temperature, at which the current begins to increase, depends significantly on the applied pressure (see Figure 4).Based on the obtained results and the information given in Table 2, the following pressing conditions were chosen for LN:Pr, LN:Mg,Pr, LT:Pr nanopowders:  powder mass-0.4g;  pressure-190 MPa;  voltage-1 kV;  temperature-200 °C.
An increase in the pressure above 190 MPa with simultaneous heating can cause an electrical breakdown of the pressed sample.Therefore, the proposed choice can be considered optimal for the configuration used in our study.
As an example, the temperature dependence of the current in the LN:Pr sample is presented in Figure 5.For pressing without the application of temperature and an electrical field, the mass of powders was 0.4 g, the pressure was 190 MPa and the pressing time was 15 min.In both modes, the thickness of the pressed sample was about 1.5 mm.Note that no binder materials were used during such pressing.
Manufacturing of ceramic tablets involves their post-pressing and high-temperature annealing, and in our case, it was performed at 600 °C for 6 h in the air.The chosen temperature was not enough to obtain very dense ceramics.However, this mode was selected for the following reasons.The main task of the work was to investigate the luminescence of LN:Pr, LN:Mg, Pr and LT:Pr nanopowders.In addition, another task was to investigate whether the luminescent properties of the studied samples are influenced by the electrical ordering of ferroelectric nanoparticles.
Therefore, the samples must be manufactured under the closest possible conditions for correct comparison of properties.It should also be noted that the transition from the ferroelectric phase to the paraelectric one in LN occurs in the temperature range of 1100-1200 °C while in LT-at temperatures above 600 °C.Consequently, the samples were annealed at 600 °C with an aim not to destroy the possible ordered state achieved by pressing with an electric field.Therefore, three tablets with the compositions of Li0.98Pr0.02NbO3,Li0.93Pr0.02Mg0.05NbO3and Li0.98Pr0.02TaO3were fabricated from structurally single-phase For pressing without the application of temperature and an electrical field, the mass of powders was 0.4 g, the pressure was 190 MPa and the pressing time was 15 min.In both modes, the thickness of the pressed sample was about 1.5 mm.Note that no binder materials were used during such pressing.
Manufacturing of ceramic tablets involves their post-pressing and high-temperature annealing, and in our case, it was performed at 600 • C for 6 h in the air.The chosen temperature was not enough to obtain very dense ceramics.However, this mode was selected for the following reasons.The main task of the work was to investigate the luminescence of LN:Pr, LN:Mg, Pr and LT:Pr nanopowders.In addition, another task was to investigate whether the luminescent properties of the studied samples are influenced by the electrical ordering of ferroelectric nanoparticles.
Therefore, the samples must be manufactured under the closest possible conditions for correct comparison of properties.It should also be noted that the transition from the ferroelectric phase to the paraelectric one in LN occurs in the temperature range of 1100-1200 • C while in LT-at temperatures above 600 • C. Consequently, the samples were annealed at 600 • C with an aim not to destroy the possible ordered state achieved by pressing with an electric field.Therefore, three tablets with the compositions of Li 0.98 Pr 0.02 NbO 3 , Li 0.93 Pr 0.02 Mg 0.05 NbO 3 and Li 0.98 Pr 0.02 TaO 3 were fabricated from structurally single-phase nanopowders with simultaneous heating and application of an electric field.Another three discs with the same compositions were prepared with no voltage or temperature applied.As an example, the picture of the LiNbO 3 :Pr sample prepared for luminescence studies is shown as an example in Figure 6.
Powders 2023, 2 570 nanopowders with simultaneous heating and application of an electric field.three discs with the same compositions were prepared with no voltage or temp applied.As an example, the picture of the LiNbO3:Pr sample prepared for lumin studies is shown as an example in Figure 6.

Photoluminescence and Photoluminescence Excitation Spectra
The photoluminescence and its excitation were studied in the red spectral similarly to the previously published investigations (e.g., [4,5]).
The excitation spectra monitored at 623 nm and the spectrum of luminescence at 270 nm of LN:Pr ceramic samples are presented in Figure 7.The spectra of obtained in two modes (during heating with the application of an electric field an out the influence of these factors) are given for comparison.In contrast to LN:Pr, the "red" luminescence in LT:Pr samples has a lower in and its excitation bands at 240 nm and 290 nm are shifted toward shorter wav (Figure 8).

Photoluminescence and Photoluminescence Excitation Spectra
The photoluminescence and its excitation were studied in the red spectral region, similarly to the previously published investigations (e.g., [4,5]).
The excitation spectra monitored at 623 nm and the spectrum of luminescence excited at 270 nm of LN:Pr ceramic samples are presented in Figure 7.The spectra of samples obtained in two modes (during heating with the application of an electric field and without the influence of these factors) are given for comparison.
three discs with the same compositions were prepared with no voltage or tem applied.As an example, the picture of the LiNbO3:Pr sample prepared for lumin studies is shown as an example in Figure 6.

Photoluminescence and Photoluminescence Excitation Spectra
The photoluminescence and its excitation were studied in the red spectra similarly to the previously published investigations (e.g., [4,5]).
The excitation spectra monitored at 623 nm and the spectrum of luminescenc at 270 nm of LN:Pr ceramic samples are presented in Figure 7.The spectra of obtained in two modes (during heating with the application of an electric field a out the influence of these factors) are given for comparison.In contrast to LN:Pr, the "red" luminescence in LT:Pr samples has a lower i and its excitation bands at 240 nm and 290 nm are shifted toward shorter wav (Figure 8).In contrast to LN:Pr, the "red" luminescence in LT:Pr samples has a lower intensity, and its excitation bands at 240 nm and 290 nm are shifted toward shorter wavelengths (Figure 8).
Note that the red luminescence in all the studied samples could be excited not only in the ultraviolet range, but also in the bands of intracenter absorption of Pr 3+ ions as well, but with lower efficiency.These bands in the region of 430-510 nm appear to be more pronounced in LT:Pr samples compared to LN:Pr (Figure 8).The luminescence and its excitation of LT:Pr is more intense in samples pressed with simultaneous temperature and electric field influence, as we observed in other samples.Note that the red luminescence in all the studied samples could be excited in the ultraviolet range, but also in the bands of intracenter absorption of Pr 3+ ions but with lower efficiency.These bands in the region of 430-510 nm appear to pronounced in LT:Pr samples compared to LN:Pr (Figure 8).The luminescence excitation of LT:Pr is more intense in samples pressed with simultaneous tempera electric field influence, as we observed in other samples.

Electrical Conductivity
The studies of electrical conductivity as a function of temperature were pe on an LN:Pr ceramic sample, obtained by pressing the corresponding nanopow the electric field applied.The impedance spectra of LN:Pr are shown for 500 an in form of Nyquist diagram in Figure 9.At 500 °C, the impedance data shows a depressed single arc semicircle.Such a depression could be attributed to the n capacitance of the samples, which corresponds to low values of the CPE expon tained from fitting of Rb-CPE equivalent circuit model to experimental data.This e value at 500 °C equals 0.81 and slightly decreases with the temperature increase ance spectra at 600 °C reveal the existence of linear region of Z''(Z') dependenc follows the semicircle intercept at lower frequencies.At this temperature, the im of the samples has been additionally measured down to 0.01 Hz in order to exam low frequency region of the ρ''(ρ') dependence in more detail.However, no ch the line slope were observed.According to [30], such peculiarity at low frequencie attributed to the electrode effect, which is typical for an ionic conductor-mobil carriers in form of ions are blocking the metal-sample interface.

Electrical Conductivity
The studies of electrical conductivity as a function of temperature were performed on an LN:Pr ceramic sample, obtained by pressing the corresponding nanopowder with the electric field applied.The impedance spectra of LN:Pr are shown for 500 and 600 • C in form of Nyquist diagram in Figure 9.At 500 • C, the impedance data shows a slightly depressed single arc semicircle.Such a depression could be attributed to the non-ideal capacitance of the samples, which corresponds to low values of the CPE exponent, obtained from fitting of R b -CPE equivalent circuit model to experimental data.This exponent value at 500 • C equals 0.81 and slightly decreases with the temperature increase.Impedance spectra at 600 • C reveal the existence of linear region of Z"(Z') dependence, which follows the semicircle intercept at lower frequencies.At this temperature, the impedance of the samples has been additionally measured down to 0.01 Hz in order to examine the low frequency region of the ρ"(ρ') dependence in more detail.However, no changes in the line slope were observed.According to [30], such peculiarity at low frequencies can be attributed to the electrode effect, which is typical for an ionic conductor-mobile charge carriers in form of ions are blocking the metal-sample interface.On the other hand, a similar behavior of Z''(Z´) dependence at low frequencies ob served in [31] for polycrystalline lithium niobate samples at temperatures above 550 °C was associated with the grain boundaries' conduction mechanism.
The electrical conductivity of LN:Pr specimen is shown in Figure 10 in the form o On the other hand, a similar behavior of Z"(Z ) dependence at low frequencies observed in [31] for polycrystalline lithium niobate samples at temperatures above 550 • C was associated with the grain boundaries' conduction mechanism.
The electrical conductivity of LN:Pr specimen is shown in Figure 10 in the form of Arrhenius plots and will be discussed in the subsequent section.The LN:Pr specimen was initially pressed at a temperature of 200 • C. On the other hand, a similar behavior of Z''(Z´) dependence at low frequen served in [31] for polycrystalline lithium niobate samples at temperatures above was associated with the grain boundaries' conduction mechanism.
The electrical conductivity of LN:Pr specimen is shown in Figure 10 in the Arrhenius plots and will be discussed in the subsequent section.The LN:Pr specim initially pressed at a temperature of 200 °C

Photoluminescence
The dominant red emission in LN:Pr specimen is caused by the transition 1 D between the levels of the Pr 3+ ion [1,[9][10][11][12].As shown in Figure 7, the red lumin excitation spectra are dominated by two broad bands with maxima near 258 and In [4], the shape of the excitation spectra of red luminescence in LiNbO3:Pr 3+ mi ders was studied depending on the degree of deviation of their composition from ometry, and it was shown that the band with a maximum near 250 nm had the intensity in stoichiometric samples.Therefore, it can be assumed that the samples in present work have stoichiometric or very close to stoichiometric composition.the photoluminescence studies of nominally undoped and magnesium-doped niobate crystals [32][33][34][35] as well as the studies of photoluminescence in micropowders of various compositions [4] allow us to assume that the lumin excitation band with a maximum near 258 nm is associated with the formation of e

Photoluminescence
The dominant red emission in LN:Pr specimen is caused by the transition 1 D 2 → 3 H 4 between the levels of the Pr 3+ ion [1,[9][10][11][12].As shown in Figure 7, the red luminescence excitation spectra are dominated by two broad bands with maxima near 258 and 345 nm.In [4], the shape of the excitation spectra of red luminescence in LiNbO 3 :Pr 3+ micropowders was studied depending on the degree of deviation of their composition from stoichiometry, and it was shown that the band with a maximum near 250 nm had the highest intensity in stoichiometric samples.Therefore, it can be assumed that the samples studied in present work have stoichiometric or very close to stoichiometric composition.Further, the photoluminescence studies of nominally undoped and magnesium-doped lithium niobate crystals [32][33][34][35] as well as the studies of photoluminescence in LN:Pr 3+ micropowders of various compositions [4] allow us to assume that the luminescence excitation band with a maximum near 258 nm is associated with the formation of electron-hole pairs near regular niobium octahedra.The band near 345 nm is attributed to the formation of such pairs near the formed octahedra, in which lithium is replaced by niobium and, in our case, possibly also by praseodymium.The red luminescence itself results from the relaxation of Pr 3+ ions excited by the recombination of electron-hole pairs.The obtained results of the luminescence spectra also agree with the other literature data obtained for LN:Pr micropowders [4].
It is also worth paying attention to how the relative intensity of photoluminescence and its excitation spectra changes depending on the pressing method of ceramic samples: the luminescence of LN:Pr ceramic samples pressed during heating in the presence of an electric field shows about 30% higher intensity compared to samples that were pressed without the influence of additional factors.This could be attributed to the higher ordering of ferroelectric nanoparticles pressed in an electric field.
The luminescence and excitation spectra for LiNbO 3 :Mg,Pr ceramic samples (pressed both in an electric field during heating and without it) are similar to those observed in LN:Pr samples.However, the luminescence intensity of LiNbO 3 :Mg,Pr was almost Powders 2023, 2 573 10 times lower than that of LN:Pr.At the same time, the obtained results are not consistent with the literature data for LN:Mg,Pr single crystals [3,36,37].According to [3,36], the appearance of magnesium in LiNbO 3 :Pr crystals of congruent composition is one of the reasons for increasing the intensity and duration of luminescence in the red region of the spectrum.However, the opposite result was observed for our samples.We note that the nanocrystalline powders obtained in the present study have a chemical composition close to stoichiometric one, and it could potentially explain the observed inconsistencies.In addition, one of the reasons for the difference between the results in this work and the previously published data [3,36,37] may be the difference in the technology employed for obtaining LN:Mg,Pr samples.Currently, we are unaware of any comparative studies of the luminescent properties performed on LN:Pr and LN:Mg,Pr single crystals, micropowders and nanopowders.
The results of the photoluminescence studies of LT:Pr nanocrystalline samples are consistent with the literature data for LiTaO 3 :Pr micropowders [5].The position of maxima and relative intensity are summarized in Table 3; Table 4 to compare the similarities and differences between the photoluminescence spectra of Pr and its excitation in LN, LN:Mg and LT nanopowders pressed under different conditions.As it can be seen from the Table 3, the highest level of luminescence and its excitation are observed for LN:Pr nanopowders pressed during heating in an electric field.
The maxima of Pr photoluminescence in LN and LN:Mg nanopowders are observed close to λ = 622 nm in all the studied samples of this type.For LT nanopowders, this maximum is located at λ = 620 nm.The UV excitation spectra of Pr 3+ ions in LN and LN:Mg powders are also similar while these maxima are noticeably shifted towards higher energies in LT specimens.

Conductivity
The obtained values of electrical conductivity (Figure 10) are generally consistent with the values obtained previously for single crystalline lithium niobate and lithium tantalate [25,33,34].The conductivity of LN:Pr specimen increases linearly in the Arrhenius presentation (see Figure 10), indicating that it is governed by a single thermally activated process.An analysis of the literature suggests that the ionic conduction mechanism with lithium vacancies as a main charge carrier determines the conductivity at elevated temperatures [25,29,[33][34][35][36][37][38].The lithium vacancy model suggests that compensation of Nb 4 Li defects occurs due to lithium vacancies.The niobium ions in the position of lithium are considered to be those point defects that participate in the processes of the capture of charge carriers and changes in the optical and electrophysical properties of LN [38].Consequently, the activation energy, E A , could be determined using the relation: where σ 0 , T, E A and k represent the pre-exponential constant, absolute temperature, activation energy and the Boltzmann constant, respectively.The activation energy obtained for LN:Pr is equal to (1.00 ± 0.05) eV.In general, this value is in a good agreement with the values, obtained previously for polycrystalline lithium niobate and/or lithium tantalate as well as for LiNb 1−x Ta x O 3 nanopowders [14,15,[39][40][41][42], ranging from 0.88 eV to 1.09 eV.Such a wide range of activation energies may be related to their strong dependence on the grain size of the samples or as well as preparation method.

Conclusions
Single-phase nanopowders with nominal compositions of Li 0.98 Pr 0.02 NbO 3 , Li 0.93 Mg 0.05 Pr 0.02 NbO 3 and Li 0.98 Pr 0.02 TaO 3 with particle sizes of 20-80 nm were obtained for the first time by high-energy milling with subsequent annealing.The absence of parasitic phases in the obtained compounds was confirmed by the XRD analysis.The pressing equipment was developed to obtain ceramic samples suitable for luminescence studies.The pressing procedure was performed in two modes: during heating with the application of an electric field and without additional factors.The studies of the photoluminescence of praseodymium ions and their excitation were carried out.It should be noted that the method of sample preparation significantly affected the sample properties.The samples pressed with the temperature and electric field show higher relative photoluminescence intensity, which could possibly be attributed to the higher ordering of ferroelectric nanoparticles in an electric field during pressing.The excitation of praseodymium ions most effectively occurs due to the recombination of electron-hole pairs formed during light absorption in the UV range.The luminescence spectra and their excitation coincide in shape and spectral position with the data for LN:Pr and LT:Pr single crystals and micropowders.At the same time, there are discrepancies in the observed luminescence intensity of nanopowders with available data for single crystals and micropowders.Such differences may be attributed to varying degrees of the chemical composition deviation from stoichiometry as well as the peculiarities of synthesis technologies.Finally, the electrical conductivity of LN:Pr sample was determined up to 670 • C in air.The dominating transport mechanism was attributed to the lithium ions migration via lithium vacancies as found in single crystalline LN.
The obtained nanopowders are of significant interest primarily as persistence luminescent materials as well as materials capable of exhibiting mechanoluminescence.This opens up prospects for their use in sensing applications (e.g., pressure, temperature, etc.).Furthermore, the relative simplicity of the nanopowders synthesis technology offers possibilities for significant cost reduction compared, for example, to obtaining a range of crystals of different compositions using the Czochralski technique.Additionally, the obtained nanocrystalline single-phase materials can serve as a raw material for obtaining corresponding thin film materials or even single crystals.

Figure 1 .
Figure 1.XRD patterns of lithium niobate (a) and the precursor obtained after milling a mixture of powders of lithium carbonate, niobium pentoxide and praseodymium oxide (b).

Figure 1 .
Figure 1.XRD patterns of lithium niobate (a) and the precursor obtained after milling a mixture of powders of lithium carbonate, niobium pentoxide and praseodymium oxide (b).

Figure 1 .
Figure 1.XRD patterns of lithium niobate (a) and the precursor obtained after milling a m powders of lithium carbonate, niobium pentoxide and praseodymium oxide (b).

Figure 2 .
Figure 2. XRD pattern of LN:Pr, LN:Pr, Mg and LT:Pr nanopowders obtained by the mechanosynthesis and annealing.

Figure 4 .
Figure 4.The temperature dependence of current in the LN sample at different pressures and 1kV electric field (for the sake of clarity, only every third data point is shown).

Figure 4 .
Figure 4.The temperature dependence of current in the LN sample at different pressures and 1 kV electric field (for the sake of clarity, only every third data point is shown).

Figure 5 .
Figure 5.The temperature dependence of current with applied pressure of 190 MPa for LN:Pr.

Figure 5 .
Figure 5.The temperature dependence of current with applied pressure of 190 MPa for LN:Pr.

Figure 7 .
Figure 7.The photoluminescence and photoluminescence excitation spectra of LiNbO3:Pr

Figure 10 .
Figure 10.Electrical conductivity of LN:Pr specimen as a function of temperature.

Figure 10 .
Figure 10.Electrical conductivity of LN:Pr specimen as a function of temperature.

Table 2 .
Conditions for obtaining ceramic samples according to the literature data.

The Preparation Method of the Powder Binder Pressure Pressure Converted into Mass for a Press Mold Ø = 10 mm Size Heat Treatment Conditions Ref.
coated with [Li 0.05 (K 0.5 Na 0.5 ) 0.95 ]NbO 3 powder in a closed Al 2 O 3 crucible before treatment.

Table 3 .
The maxima position and relative intensity of the Pr luminescence excitation spectra at a wavelength of λ = 623 nm in LN:Pr, LN:Mg,Pr and LT:Pr nanopowders.

Table 4 .
The position of the photoluminescence maxima of praseodymium and its relative intensity in LN:Pr, LN:Mg,Pr and LT:Pr nanopowders.