Spectroscopic Properties of Inorganic Glasses Doped with Pr3+: A Comparative Study

The results presented in this communication concern visible and near-IR emission of Pr3+ ions in selected inorganic glasses, i.e., borate-based glass with Ga2O3 and BaO, lead-phosphate glass with Ga2O3, gallo-germanate glass modified by BaO/BaF2, and multicomponent fluoride glass based on InF3. Glasses present several emission bands at blue, reddish orange, and near-infrared spectral ranges, which correspond to 4f–4f electronic transitions of Pr3+. The profiles of emission bands and their relative intensity ratios depend strongly on glass-host. Visible emission of Pr3+ ions is tuned from red/orange for borate-based glass to nearly white light for multicomponent fluoride glass based on InF3. The positions and spectral linewidths for near-infrared luminescence bands at the optical telecommunication window corresponding to the 1G4 → 3H5, 1D2 → 1G4, and 3H4 → 3F3,3F4 transitions of Pr3+ are dependent on glass-host matrices and excitation wavelengths. Low-phonon fluoride glasses based on InF3 and gallo-germanate glasses with BaO/BaF2 are excellent candidates for broadband near-infrared optical amplifiers. Spectroscopic properties of Pr3+-doped glasses are compared and discussed in relation to potential optical applications.

Here we present comparative studies on selected inorganic glasses containing Pr 3+ , i.e., borate glass with Ga 2 O 3 and BaO, lead-phosphate glass with Ga 2 O 3 , gallo-germanate glass modified by BaO/BaF 2 , and multicomponent fluoride glass based on InF 3 . Based on luminescence spectra and their decays, several spectroscopic parameters of Pr 3+ ions were determined. Previous investigations illustrated quite well the relationship between the structural modifications of glasses and their emission and spectroscopic properties. For example, several glass-modifiers were introduced to borate glasses doped with Pr 3+ ions. Anjaiah et al. [37] studied luminescence properties of Pr 3+ -doped lithium borate glasses modified by MO (where M = Zn, Ca, Cd). Based on some spectroscopic parameters such as the Judd-Ofelt intensity parameter Ω 2 and the bonding parameter δ, it was suggested that Selected inorganic glasses doped with Pr 3+ ions were synthesized using traditional high-temperature melt-quenching technique. Their chemical compositions and melting conditions are given in Table 1. For the studied glass samples, the activator concentration was the same (0.1 mol%). Pr 3+ -doped lead-phosphate glass with Ga 2 O 3 (PPG-Pr) was also selected to study reddish orange emission varying with activator concentration. Samples of PPG-Pr with various Pr 3+ concentrations were prepared. They are given in Table 2. The appropriate precursor metal oxides and/or fluorides of high purity (99.99%) were mixed in a Pt crucible and then melted in a special glove-box in an Ar atmosphere. Glass samples with dimension = 10 mm × 10 mm and thickness = 2 mm were obtained. In the next step, absorption and luminescence measurements were carried out. The UV-VIS-NIR spectrophotometer (Cary 5000, Agilent Technology, Santa Clara, CA, USA) was used to measure absorption spectra. Luminescence spectra and their decays were registered

Results and Discussion
Five glass-host matrices given in Table 1 and referred to as IZSBGL-Pr, GBFG-Pr, GBG-Pr, PPG-Pr, and BBG-Pr were selected for comparative spectroscopic investigations. It should be noted that all glass samples were obtained under the same experimental conditions in order to compare their spectroscopic properties. It is well known that the conditions of synthesis are more restrictive for pure fluoride glasses in contrast to oxide glass systems. In our case, all samples were prepared in a glove-box under an atmosphere of dry argon (O 2 , H 2 O < 0.5 ppm). This procedure is especially important for IZSBGL-Pr, due to fluorine evaporation during the glass synthesis. For that reason, a small amount of ammonium bifluoride (NH 4 HF 2 ) as a fluorinating agent was also added before melting. Unfortunately, the actual concentration of fluorine ions has not been estimated. The final composition of IZSBGL-Pr may be somewhat different from the nominal starting one due to fluorine losses during the melting process. Previously published works suggest that the fluorine losses could be quite large [48][49][50][51][52]. An another important factor that effectively quenched the luminescence is the concentration of OHgroups, which can be calculated from the transmittance spectrum. Figure 1 shows transmittance spectra measured for glass samples in the 3950-2950 cm −1 frequency region. The absorption band centered at about 3400 cm −1 is ascribed to the vibration of OHgroups.
In the next step, absorption and luminescence measurements were carried out. The UV-VIS-NIR spectrophotometer (Cary 5000, Agilent Technology, Santa Clara, CA, USA) was used to measure absorption spectra. Luminescence spectra and their decays were registered using a VIS/NIR laser system. The laser equipment consisted of a Photon Technology International (PTI) Quanta-Master 40 (QM40) UV/VIS Steady State Spectrofluorometer (Photon Technology International, Birmingham, NJ, USA) coupled with tunable pulsed optical parametric oscillator (OPO), pumped by a third harmonic of a Nd:YAG laser (Opotek Opolette 355 LD, OPOTEK, Carlsband, CA, USA), xenon lamp as a light source, double 200 mm monochromator, multimode UVVIS PMT R928 detector (PTI Model 914), and Hamamatsu H10330B-75 detector (Hamamatsu, Bridgewater, NJ, USA). Resolution for spectra measurements was ±0.2 nm. Decays were measured with an accuracy of ±2 µs. Transmittance spectra were performed on the Nicolet iS50 ATR spectrometer (Thermo Fisher Scientific Instruments, Waltham, MA, USA).

Results and Discussion
Five glass-host matrices given in Table 1 and referred to as IZSBGL-Pr, GBFG-Pr, GBG-Pr, PPG-Pr, and BBG-Pr were selected for comparative spectroscopic investigations. It should be noted that all glass samples were obtained under the same experimental conditions in order to compare their spectroscopic properties. It is well known that the conditions of synthesis are more restrictive for pure fluoride glasses in contrast to oxide glass systems. In our case, all samples were prepared in a glove-box under an atmosphere of dry argon (O2, H2O < 0.5 ppm). This procedure is especially important for IZSBGL-Pr, due to fluorine evaporation during the glass synthesis. For that reason, a small amount of ammonium bifluoride (NH4HF2) as a fluorinating agent was also added before melting. Unfortunately, the actual concentration of fluorine ions has not been estimated. The final composition of IZSBGL-Pr may be somewhat different from the nominal starting one due to fluorine losses during the melting process. Previously published works suggest that the fluorine losses could be quite large [48][49][50][51][52]. An another important factor that effectively quenched the luminescence is the concentration of OHgroups, which can be calculated from the transmittance spectrum. Figure 1 shows transmittance spectra measured for glass samples in the 3950-2950 cm −1 frequency region. The absorption band centered at about 3400 cm −1 is ascribed to the vibration of OHgroups.  For fluoride glass based on InF 3 , the concentration of OHgroups is extremely low. The absorption coefficient and content of hydroxyl groups are close to 0.088 cm −1 and  3.82 ppm [53], respectively. The reduced concentration of hydroxyl groups is necessary to obtain pure fluoride glass with relatively high quantum efficiency and to enhance near-IR and mid-IR emission [54]. Further investigations indicate that the band intensity of hydroxyl groups is considerably smaller for mixed oxyfluoride gallo-germanate glass with BaF 2 (GBFG-Pr) than oxide glass (GBG-Pr). The residual absorption of OHgroups is reduced drastically in gallo-germanate glass, where BaO was replaced by BaF 2 [55]. These aspects are also important for phosphate glasses due to the hygroscopic nature of P 2 O 5 . The concentration of hydroxyl groups is usually higher in phosphate glass compared to other oxide glasses. Our recent studies for the lead-phosphate system [56] clearly demonstrated that the intensity of the IR band related to vibration of hydroxyl groups is considerably lower for glass samples synthesized in glove-box than in open air. These phenomena are very important from the optical point of view. Based on our published works [56][57][58][59], different physicochemical properties of the studied Pr 3+ -doped glasses are also summarized in Table 3. Table 3. Different physicochemical properties of the studied Pr 3+ -doped inorganic glasses [56][57][58][59]. From the average molecular weight, density, Pr 3+ ion concentration, and refractive index exhibited in Table 3, various other radiative parameters were calculated. The three phenomenological intensity parameters Ω t (where t = 2, 4, 6) were calculated by using the appropriate relations from the Judd-Ofelt (J-O) theory. In particular, the J-O intensity parameter Ω 2 is attributed to the sensitivity to the local glass structure of the rare earth sites. It is affected by symmetry/asymmetry sites and covalent/ionic bonding character between Pr 3+ ions and the nearest surroundings. In other words, the lower values of Ω 2 suggest a higher degree of ionic bonding between rare earth ions and their ligands. It is clearly seen that the value of Ω 2 is greater for glass GBG-Pr, in contrast to fluoride glass IZSBGL-Pr and oxide glasses assigned to PPG-Pr and BBG-Pr, suggesting a higher degree of covalence between Pr 3+ ions and the surrounding ligands. Independently of glass-host, the radiative transition rates obtained from the J-O calculations are significantly higher for the 3 P 0 state than the lower-lying 1 D 2 state of Pr 3+ ions. Further calculations from the relevant expression η = τ m /τ rad × 100% (τ m and τ rad are measured and radiative lifetime, respectively, calculated from the J-O theory) indicate that the quantum efficiency for the excited state 1 D 2 (Pr 3+ ) is significantly larger for low-phonon oxide (GBG-Pr) and fluoride (IZSBGL-Pr) glasses, confirming their suitability for near-infrared luminescence applications. Glass transition temperature T g for the studied glass-host matrices was also determined from DSC curve measurements. The value of T g is much lower for fluoride glass IZSBGL-Pr compared to other systems. Glass GBG-Pr is characterized by the highest glass transition temperature among the studied glass systems. It is also interesting to note that the value of T g changes from 620 • C (GBG-Pr) to 599 • C (GBFG-Pr) in gallo-germanate glass where BaO was partially substituted by BaF 2 [59]. Furthermore, the energy level diagram for Pr 3+ ions schematized in Figure 2 favors several visible and near-infrared emission transitions. respectively, calculated from the J-O theory) indicate that the quantum efficiency for the excited state 1 D2 (Pr 3+ ) is significantly larger for low-phonon oxide (GBG-Pr) and fluoride (IZSBGL-Pr) glasses, confirming their suitability for near-infrared luminescence applications. Glass transition temperature Tg for the studied glass-host matrices was also determined from DSC curve measurements. The value of Tg is much lower for fluoride glass IZSBGL-Pr compared to other systems. Glass GBG-Pr is characterized by the highest glass transition temperature among the studied glass systems. It is also interesting to note that the value of Tg changes from 620 °C (GBG-Pr) to 599 °C (GBFG-Pr) in gallo-germanate glass where BaO was partially substituted by BaF2 [59]. Furthermore, the energy level diagram for Pr 3+ ions schematized in Figure 2 favors several visible and near-infrared emission transitions. The spectroscopic results for Pr 3+ ions in fluoride glass based on InF3 (IZSBGL-Pr), borate glass with Ga2O3 and BaO (BBG-Pr), lead-phosphate glass with Ga2O3 (PPG-Pr), and gallo-germanate glassses modified by BaO/BaF2 (referred to as GBG-Pr and GBFG-Pr) are presented and discussed here. Figure 3 presents absorption (a,b) and visible emission (c,d) spectra and emission decays (e,f) from 1 D2 state of Pr 3+ ions in the studied glass systems. Absorption spectra consist of characteristic bands which correspond to transitions originating from ground state 3 H4 to the higher-lying excited states of praseodymium ions. The most intense bands centered at 445 nm and 590 nm are related to 3 H4 → 3 P2 and 3 H4 → 1 D2 transitions of Pr 3+ , respectively. The UV cut-off wavelength, defined as the intersection between the zero baseline and the extrapolation of absorption edge, is located in the 300-350 nm range. In general, the absorption edge is shifted to shorter wavelengths from oxide borate glass BBG-Pr to fluoride glass IZSBGL-Pr. Visible emission spectra were excited at 3 P2 state (λexc = 445 nm) and show several characteristic bands of Pr 3+ ions. The most intense bands are located in the blue and reddish orange spectral ranges and correspond to 3 P0 → 3 H4, 1 D2 → 3 H4, 3 P0 → 3 H6, and 3 P0 → 3 F2 electronic transitions of Pr 3+ . The spectroscopic results for Pr 3+ ions in fluoride glass based on InF 3 (IZSBGL-Pr), borate glass with Ga 2 O 3 and BaO (BBG-Pr), lead-phosphate glass with Ga 2 O 3 (PPG-Pr), and gallo-germanate glassses modified by BaO/BaF 2 (referred to as GBG-Pr and GBFG-Pr) are presented and discussed here. Figure 3 presents absorption (a,b) and visible emission (c,d) spectra and emission decays (e,f) from 1 D 2 state of Pr 3+ ions in the studied glass systems. Absorption spectra consist of characteristic bands which correspond to transitions originating from ground state 3 H 4 to the higher-lying excited states of praseodymium ions. The most intense bands centered at 445 nm and 590 nm are related to 3 H 4 → 3 P 2 and 3 H 4 → 1 D 2 transitions of Pr 3+ , respectively. The UV cut-off wavelength, defined as the intersection between the zero baseline and the extrapolation of absorption edge, is located in the 300-350 nm range. In general, the absorption edge is shifted to shorter wavelengths from oxide borate glass BBG-Pr to fluoride glass IZSBGL-Pr. Visible emission spectra were excited at 3 P 2 state (λ exc = 445 nm) and show several characteristic bands of Pr 3+ ions. The most intense bands are located in the blue and reddish orange spectral ranges and correspond to 3 P 0 → 3 H 4 , 1 D 2 → 3 H 4 , 3 P 0 → 3 H 6 , and 3 P 0 → 3 F 2 electronic transitions of Pr 3+ .

IZSBGL-Pr GBG-Pr PPG-Pr BBG-Pr
Further analysis demonstrates that the relative integrated intensities of emission bands located in the blue and reddish orange region are completely different and depend strongly on kind of glass-host. Previous studies revealed that fluorescence intensity ratio, referred to as red-to-blue R/B [60] or orange-to-blue O/B [61], decreases with increasing Pr 3+ ion concentration. In our case, fluorescence intensity ratio I REDDISH-ORANGE /I BLUE varying with glass-host was also estimated and schematized in Figure 3. This factor is enhanced rapidly from fluoride glass IZSBGL-Pr to borate-based glass BBG-Pr, due to the increase in the non-radiative rates. As a consequence, the 3 P 0 state is depopulated very quickly, and the excitation energy is transferred non-radiatively to the lower-lying state 1 D 2 (Pr 3+ ). It can be well explained by the phonon energy of the host (Table 3), which increases from 510 cm −1 (IZSBGL-Pr) to 1400 cm −1 (BBG-Pr). Thus, high-phonon borate glass BBG-Pr is favored to bridge the energy gap between 3 P 0 and 1 D 2 states of Pr 3+ ions, and reddish orange emission due to 1 D 2 → 3 H 4 transition is dominant. This was also confirmed by luminescence decay analysis. The multi-phonon relaxation rates of Pr 3+ increase with increasing phonon energy from IZSBGL-Pr to BBG-Pr. Owing to higher multi-phonon relaxation rates, the measured luminescence lifetimes of 1 D 2 (Pr 3+ ) are reduced from fluoride glass IZSBGL-Pr to boratebased glass BBG-Pr. Furthermore, luminescence decays from 1 D 2 state in all glass samples containing 0.1 mol% Pr 3+ ions are mono-exponential. According to the excellent review article published recently by Tanner et al. [62], mono-exponential decay using the Förster expression for W ET can be given for electric-dipole type transfer by: or the following relation: where R 0 is critical transfer distance (also called Förster radius), R is the average interionic separation, equal to (3/4πN) 1/3 , and N denotes activator concentration.  Further analysis demonstrates that the relative integrated intensities of emission bands located in the blue and reddish orange region are completely different and depend strongly on kind of glass-host. Previous studies revealed that fluorescence intensity ratio, referred to as red-to-blue R/B [60] or orange-to-blue O/B [61], decreases with increasing Pr 3+ ion concentration. In our case, fluorescence intensity ratio IREDDISH-ORANGE/IBLUE varying with glass-host was also estimated and schematized in Figure 3. This factor is enhanced rapidly from fluoride glass IZSBGL-Pr to borate-based glass BBG-Pr, due to the increase in the non-radiative rates. As a consequence, the 3 P0 state is depopulated very quickly, and the excitation energy is transferred non-radiatively to the lower-lying state 1 D2 (Pr 3+ ). It can be well explained by the phonon energy of the host (Table 3), which increases from 510 cm −1 (IZSBGL-Pr) to 1400 cm −1 (BBG-Pr). Thus, high-phonon borate glass BBG-Pr is favored to bridge the energy gap between 3 P0 and 1 D2 states of Pr 3+ ions, and reddish orange emission due to 1 D2 → 3 H4 transition is dominant. This was also confirmed by luminescence decay analysis. The multi-phonon relaxation rates of Pr 3+ increase with increasing phonon energy from IZSBGL-Pr to BBG-Pr. Owing to higher multi-phonon relaxation rates, the measured luminescence lifetimes of 1 D2 (Pr 3+ ) are reduced from fluoride glass IZSBGL-Pr to borate-based glass BBG-Pr. Furthermore, luminescence decays from 1 D2 The energy transfer and cross-relaxation processes are neglected when the average interionic separation R between Pr 3+ ions is greater than the critical transfer distance R 0 . Our studies clearly indicate that calculated values of R for all studied glass-host matrices containing 0.1 mol% Pr 3+ ions are greater than the Förster distances R 0 (Table 3). Previous results obtained for Pr 3+ -doped ZBLAN fluoride glass suggest that the average distance is smaller than the critical transfer distance and the energy transfer process will promote the non-exponential decay from the 1 D 2 state for activator (Pr 3+ ) content ≥ 0.5 mol% [63].
Among inorganic glass systems, it is also found that the measured 1 D 2 luminescence lifetime is longer than the 3 P 0 lifetime of Pr 3+ ions. This was confirmed by luminescence decay curve measurements for Pr 3+ ions in multicomponent fluoro-phosphate glasses [15], oxyfluoroborate glasses [17], lead germanate glasses [23], and borosilicate glasses [61] as well as tellurite [64] and zinc telluro-fluoroborate [65] glass systems. Luminescence lifetimes for 3 P 0 and 1 D 2 states of Pr 3+ ions in different glass-host matrices are presented in Table 4. Also, the x and y of CIE chromaticity coordinates for IZSBGL-Pr, GBFG-Pr, GBG-Pr, PPG-Pr, and BBG-Pr systems were calculated from the emission spectra. The results are given in Table 5. They are shown in the chromaticity diagram in Figure 4.    Spectroscopic studies indicate that PPG-Pr and BBG-Pr belong to inorganic glasses emitting reddish orange emission, similar to other lead-free and lead-based [66][67][68][69] glass systems doped with Pr 3+ published recently. It is noteworthy that the color of emission is changed from reddish orange (BGB-Pr) to yellowish orange (BGFG-Pr) where BaO was replaced by BaF2 (5 mol%). Based on the CIE diagram, we can conclude that emission can be tuned from red/orange (BBG-Pr) to nearly white light region (IZSBGL-Pr) by changing Spectroscopic studies indicate that PPG-Pr and BBG-Pr belong to inorganic glasses emitting reddish orange emission, similar to other lead-free and lead-based [66][67][68][69] glass systems doped with Pr 3+ published recently. It is noteworthy that the color of emission is changed from reddish orange (BGB-Pr) to yellowish orange (BGFG-Pr) where BaO was replaced by BaF 2 (5 mol%). Based on the CIE diagram, we can conclude that emission can be tuned from red/orange (BBG-Pr) to nearly white light region (IZSBGL-Pr) by changing chromaticity parameters by varying the glass-host matrix.

Glass Code CIE Chromaticity Coordinates
Our previous investigations suggested that the spectral profiles of emission bands of Pr 3+ ions and their relative intensity ratios are changed during modification of glass-host. In the orange-red region, two emission bands due to 1 D 2 → 3 H 4 (orange) and 3 P 0 → 3 H 6 (red) transitions of Pr 3+ are overlapped, and their intensities depend strongly on the glass-host. This was well evidenced for gallo-germanate glasses modified by BaO/BaF 2 [70]. Figure 5 shows reddish orange emission spectra dependent on glass-host matrix and Pr 3+ content. Spectroscopic studies indicate that PPG-Pr and BBG-Pr belong to inorganic glasses emitting reddish orange emission, similar to other lead-free and lead-based [66][67][68][69] glass systems doped with Pr 3+ published recently. It is noteworthy that the color of emission is changed from reddish orange (BGB-Pr) to yellowish orange (BGFG-Pr) where BaO was replaced by BaF2 (5 mol%). Based on the CIE diagram, we can conclude that emission can be tuned from red/orange (BBG-Pr) to nearly white light region (IZSBGL-Pr) by changing chromaticity parameters by varying the glass-host matrix.
Our previous investigations suggested that the spectral profiles of emission bands of Pr 3+ ions and their relative intensity ratios are changed during modification of glass-host. In the orange-red region, two emission bands due to 1 D2 → 3 H4 (orange) and 3 P0 → 3 H6 (red) transitions of Pr 3+ are overlapped, and their intensities depend strongly on the glasshost. This was well evidenced for gallo-germanate glasses modified by BaO/BaF2 [70]. Figure 5 shows reddish orange emission spectra dependent on glass-host matrix and Pr 3+ content.  From literature data, it is well known that multi-phonon relaxation (MPR) and cross relaxation (CR) processes play an important role in population or depopulation of the 1 D 2 state of Pr 3+ ions in inorganic glasses. The non-radiative transition rate W nr due to the MPR process is equal to 2.47 × 10 4 s −1 for glass based on InF 3 [71], whereas the value of W nr for borate glass is approximately 10 3 times larger than that of the fluoride glass system [72]. The phonon energy of the host increases from IZSBGL-Pr to BBG-Pr. Thus, the excitation energy is transferred more efficiently from the higher-lying 3 P 0 state to the 1 D 2 state, and, consequently, reddish orange luminescence corresponding to 1 D 2 → 3 H 4 transition of Pr 3+ in borate-based glass (BBG-Pr) is dominant, as mentioned above. This situation is observed for glasses when the molar concentration of Pr 3+ ions is relatively low and its value is close to 0.1 mol%. It is generally accepted that the MPR process from the 3 P 0 state at lower concentrations (usually below 0.5 mol%) favors reddish orange emission from the 1 D 2 state to be more dominant [61]. For higher activator concentrations (above 0.5 mol%), the nonradiative energy transfer processes between Pr 3+ ions become efficient, and luminescence associated to 1 D 2 → 3 H 4 transition is successfully quenched through cross-relaxation. The following CR processes, 1 D 2 : 3 H 4 → 1 G 4 : ( 3 F 3 , 3 F 4 ) and 1 D 2 : 3 H 4 → ( 3 F 3 , 3 F 4 ): 1 G 4 , are responsible for depopulation of the 1 D 2 state of Pr 3+ [73]. In addition, these aspects have been examined by us. In our case, lead-phosphate glass (PPG-Pr) was selected as an intermediate medium, in which luminescence from both 3 P 0 and 1 D 2 states of Pr 3+ ions are well observed and the 1 D 2 → 3 H 4 transition is dominant at low activator concentration. The results are presented in Figure 5b. It is well evidenced that the emission intensity of 1 D 2 → 3 H 4 transition is reduced, whereas the emission intensities of bands originating from the 3 P 0 state are enhanced with increasing Pr 3+ concentration. These phenomena are associated with Pr 3+ -Pr 3+ interaction increasing and the presence of cross-relaxation processes at higher activator concentration. A similar situation was observed for zinctelluro-fluoroborate glass examined as a function of Pr 3+ ion concentration [66]. Our experimental results evidently suggest that the contribution of the glass-host to the change in the spectral factor I REDDISH-ORANGE /I BLUE and measured lifetime ( Figure 3) seems to be dominant when content of Pr 3+ is relatively low (0.1 mol%). In this case, the multi-phonon relaxation process makes an important contribution to the excited state relaxation of Pr 3+ (Figure 5a). The situation was completely changed when concentration of rare earths was relatively high (Figure 5b). Thus, the contribution of activator content was dominant. This behavior is due to the presence of non-radiative energy transfer processes (such as crossrelaxation), which contribute to quenching of luminescence corresponding to 1 D 2 → 3 H 4 transition of Pr 3+ . Figure 6 presents near-infrared emission spectra of Pr 3+ ions in inorganic glasses, which were excited at 445 nm ( 3 P 0 ) and 590 nm ( 1 D 2 ), respectively. In order to compare luminescence linewidth, defined as full width at half maximum (FWHM), the spectra measured in the 1200-1650 nm range were also normalized.  Independently of excitation wavelengths, broadband near-infrared emission bands (FWHM above 200 nm) are observed for BBG-Pr, GBG, and GBFG glasses. From the literature, it is well known that near-infrared luminescence properties of glasses containing Pr 3+ ions depend strongly on the excitation wavelengths. The blue and orange excitation lines are unusually helpful to examine conversion of blue light into near-infrared radiation and its mechanism. These processes have been observed for some fluoride materials and other low-phonon systems. The experimental results for glass-ceramic materials with CaF2:Pr 3+ nanocrystals [76] indicated that a two-step near-infrared quantum cutting (NIR-QC) from blue-excited 3 P0 state takes place efficiently, with 1 G4 acting as an intermediate state. Blue light excitation leading to efficient population of 1 G4 state also influences the relative integrated intensities of emission bands, which correspond to near-infrared transitions originating from both 1 D2 and 1 G4 states of Pr 3+ . A tunable amplification band depending on the excitation wavelength used (474 nm/980 nm) has been also observed for Pr 3+ /Yb 3+ co-doped systems, where it is possible to select 1 D2 → 1 G4 or 1 G4 → 3 H5 transition of Pr 3+ . When the excitation wavelength was changed from 474 nm to 980 nm, the nearinfrared luminescence switched from the E-S bands near 1480 nm to the O-E bands centered at 1330 nm in Pr 3+ /Yb 3+ co-doped tellurite tungstate glasses [77]. The near-infrared luminescence spectra show several bands which correspond to 1 D 2 → 3 F 3 , 3 F 4 , 1 G 4 → 3 H 5 , 1 D 2 → 1 G 4 , and 3 H 4 → 3 F 3 , 3 F 4 transitions of Pr 3+ , respectively. Their relative integrated emission intensities are changed drastically with glass-host matrices. In particular, luminescence bands located in the so-called telecom window (1200-1650 nm) have been examined in detail. In this spectral range, ultra-broadband near-infrared emission of Pr 3+ ions related to 1 G 4 → 3 H 5 (λ p = 1330 nm) and 1 D 2 → 1 G 4 (λ p = 1480 nm) transitions is observed for several inorganic glasses, which is extremely useful for optical fiber amplifiers operating at E-, S-, C-, and L-band [74]. In some cases, a near-infrared emission band centered at about 1600 nm is also visible. This emission band is connected with the 3 H 4 → 3 F 3 , 3 F 4 transition of Pr 3+ [75]. Interesting results are observed for fluoride glass IZSBGL-Pr. In contrast to other studied glass systems, the intensities of emission bands of Pr 3+ ions in glass IZSBGL-Pr, covering a spectral range from 1200 nm to 1650 nm, depend also on the excitation wavelengths (445 nm/590 nm). When glass IZSBGL-Pr was excited at 445 nm ( 3 P 2 ), the intensities of bands were extremely low, and the near-infrared emission near 1335 nm due to the 1 G 4 → 3 H 5 transition was dominant. The situation changed when the glass sample was excited at 590 nm ( 1 D 2 ). Thus, the near-infrared emission in glass IZSBGL-Pr is the most intense, and the 1 D 2 → 1 G 4 transition centered at about 1450 nm is dominant.
Independently of excitation wavelengths, broadband near-infrared emission bands (FWHM above 200 nm) are observed for BBG-Pr, GBG, and GBFG glasses. From the literature, it is well known that near-infrared luminescence properties of glasses containing Pr 3+ ions depend strongly on the excitation wavelengths. The blue and orange excitation lines are unusually helpful to examine conversion of blue light into near-infrared radiation and its mechanism. These processes have been observed for some fluoride materials and other low-phonon systems. The experimental results for glass-ceramic materials with CaF 2 :Pr 3+ nanocrystals [76] indicated that a two-step near-infrared quantum cutting (NIR-QC) from blue-excited 3 P 0 state takes place efficiently, with 1 G 4 acting as an intermediate state. Blue light excitation leading to efficient population of 1 G 4 state also influences the relative integrated intensities of emission bands, which correspond to near-infrared transitions originating from both 1 D 2 and 1 G 4 states of Pr 3+ . A tunable amplification band depending on the excitation wavelength used (474 nm/980 nm) has been also observed for Pr 3+ /Yb 3+ co-doped systems, where it is possible to select 1 D 2 → 1 G 4 or 1 G 4 → 3 H 5 transition of Pr 3+ . When the excitation wavelength was changed from 474 nm to 980 nm, the near-infrared luminescence switched from the E-S bands near 1480 nm to the O-E bands centered at 1330 nm in Pr 3+ /Yb 3+ co-doped tellurite tungstate glasses [77].
Finally, some spectroscopic parameters for Pr 3+ ions were determined. One of the most important radiative parameters is the peak stimulated emission cross-section σ em , which can be calculated using the expression: where λ p is the peak emission wavelength, n-the refractive index, c-the velocity of light, ∆λ-the emission linewidth (FWHM), and A J -the calculated radiative transition rate from the J-O theory. The values of n and A J are given in Table 3. It is generally accepted that a relatively large value of σ em is demanded for an efficient laser transition.
In the next step, the stimulated emission cross-section (σ em ), the measured emission lifetime (τ m ), and the emission linewidth (FWHM) were applied to calculate the following parameters: figure of merit FOM (σ em × τ m ) and gain bandwidth (σ em × FWHM product). The results for the 1 D 2 → 1 G 4 transition of Pr 3+ ions in the glass systems excited at 590 nm are given in Table 6. The peak stimulated emission cross-section for PPG-Pr close to σ em = 1.28 × 10 −20 cm 2 is relatively large and comparable to the values 1.14 × 10 −20 cm 2 [78] and 1.29 × 10 −20 cm 2 [79] reported previously for similar phosphate-based glasses doped with Pr 3+ . The smaller values of the stimulated emission cross-section (σ em = 0.5 × 10 −20 cm 2 ) as well as the gain bandwidth (σ em × FWHM = 65 × 10 −27 cm 3 ) for fluoride glass IZSBGL-Pr are mainly due to the considerably lower spectral linewidth for 1 D 2 → 1 G 4 transition of Pr 3+ . On the other hand, the figure of merit (FOM) for IZSBGL-Pr is the highest among the studied glass systems.
The peak stimulated emission cross-section, the figure of merit (FOM), and the gain bandwidth seem to be considerably smaller for glass BBG-Pr, due to its relatively large nonradiative transition rate. For that reason, high-phonon borate-based glass BBG-Pr is useless for near-infrared luminescence applications. The σ em × FWHM product, as an important parameter to achieve broadband and high gain amplification, is quite large for GBG and GBFG glasses (above 200 × 10 −27 cm 3 ). Their calculated values are comparable to the one (174.6 × 10 −27 cm 3 ) obtained for the 1 D 2 → 1 G 4 transition of Pr 3+ ions in fluorotellurite glass [80], demonstrating suitability for broadband near-infrared amplifiers.

Conclusions
In this work, comparative spectroscopic properties of selected inorganic glasses singly doped with Pr 3+ ions are reported. The experimental results were limited to borate-based glass with Ga 2 O 3 and BaO, lead-phosphate glass with Ga 2 O 3 , gallo-germanate glass modified by BaO/BaF 2 , and multicomponent fluoride glass based on InF 3 . Spectroscopic parameters for Pr 3+ ions in glass samples were determined based on absorption/emission spectra measurements and emission decay curve analysis. Emission spectra at visible and near-infrared wavelengths were analyzed based on the energy level diagram of Pr 3+ . The systematic studies revealed that profiles of emission bands and their relative integrated intensity ratios depend significantly on glass-host matrices. Visible emission of Pr 3+ is modulated from red/orange for borate-based glass and lead-phosphate glass with Ga 2 O 3 via yellowish orange for gallo-germanate glass with BaO/BaF 2 to nearly white light for fluoride glass based on InF 3 . The band positions and spectral linewidths for near-infrared luminescence at telecom range associated with the 1 G 4 → 3 H 5 , 1 D 2 → 1 G 4 , and 3 H 4 → 3 F 3 , 3 F 4 transitions of Pr 3+ are influenced by the kind of glass matrix and excitation wavelengths. Based on several spectroscopic parameters of Pr 3+ ions, it was suggested that low-phonon fluoride glasses based on InF 3 and gallo-germanate glasses with BaO/BaF 2 are promising materials for optical amplification. The results are compared and discussed in relation to potential applications as multicolor visible light sources or broadband near-infrared optical amplifiers.

Data Availability Statement:
The data presented in this study are available on request from the corresponding author.