Yttrium zinc lithium alumino antimony sodalime borosilicate glasses containing Pr3+ in (20-x):SiO2:10ZnO: 10Li2O :10Al2O3 :10Sb2O3 :10Na2O :10CaO :10Y2O3 :10B2O3:xPr2O3 (where x=1, 1.5,2 mol %) have been prepared by melt-quenching method. The amorphous nature of the glasses was confirmed by x-ray diffraction studies. DTA curve was analysed to evaluate the glass transition temperature, crystallization temperature and melting temperature. Optical absorption, Excitation spectra and fluorescence spectra were recorded at room temperature for all glass samples. Judd-Ofelt intensity parameters ?? (?=2, 4, 6) are evaluated from the intensities of various absorption bands of optical absorption spectra. Using these intensity parameters various radiative properties like spontaneous emission probability, branching ratio, radiative life time and stimulated emission cross–section of various emission lines have been evaluated.
Introduction
This study investigates the structural, thermal, and spectroscopic properties of Pr³?-doped yttrium zinc lithium alumino antimony sodalime borosilicate (YZLAASLBS) glasses prepared by the melt-quenching technique. Rare-earth-doped silicate glasses are important materials for applications in optical fiber amplifiers, lasers, frequency converters, sensors, and other optoelectronic devices because of their excellent optical transparency, thermal stability, mechanical strength, and high rare-earth ion solubility.
Glass Preparation
Three Pr³?-doped glass compositions containing 1.0, 1.5, and 2.0 mol% Pr?O? were synthesized using high-purity oxide powders. The mixed batches were melted at 1050°C, quenched on a preheated steel plate, and annealed at 350°C to remove internal stresses. The resulting samples were transparent and exhibited good optical quality.
Theoretical Analysis
The optical properties were analyzed using:
Oscillator strength calculations from absorption spectra.
Judd–Ofelt (J–O) theory, which provides intensity parameters (Ω?, Ω?, Ω?) related to the local environment and bonding around Pr³? ions.
Calculation of radiative parameters such as:
Spontaneous emission probability,
Radiative lifetime,
Fluorescence branching ratio,
Stimulated emission cross-section.
Nephelauxetic ratio and bonding parameters were used to evaluate the nature of rare-earth–oxygen bonding.
Results
1. XRD Analysis
X-ray diffraction patterns showed only broad diffuse humps and no sharp Bragg peaks.
This confirms that the prepared glasses are amorphous in nature.
2. Raman Spectroscopy
Raman bands were observed at 600, 795, and 1205 cm?¹.
These bands correspond to:
Si–O–Si symmetric stretching (600 cm?¹),
Bending vibrations (795 cm?¹),
Si–O–Si asymmetric stretching (1205 cm?¹).
The results confirm the silicate glass network structure.
3. Thermal Properties
Differential Thermal Analysis (DTA) was used to determine thermal parameters.
Pr?O? Content (mol%)
Tg (°C)
Tc (°C)
Tm (°C)
Trg
1.0
375
508
685
0.547
1.5
380
510
688
0.552
2.0
386
513
693
0.557
Key observations:
Glass transition temperature (Tg) increases with increasing Pr³? concentration.
Crystallization (Tc) and melting temperatures (Tm) also increase slightly.
The glasses exhibit good thermal stability and glass-forming ability, making them suitable for optical applications.
Conclusion
In the present study, the glass samples of composition (20-x):SiO2:10ZnO :10Li2O :10Al2O3 :10Sb2O3 :10Na2O :10CaO :10Y2O3 :10B2O3:xPr2O3 (where x =1, 1.5, 2 mol %) have been prepared by melt-quenching method. Balaji and Shankar parameters indicate that the prepared glass samples have good thermal stability.
The stimulated emission cross-section (?p) has highest value for the transition (1G4?3H6) in all the glass specimen doped with Pr3+ion. This shows that (1G4?3H6) transition is most probable transition and it useful for display device applications.
References
[1] Meena,S.L.(2026).Spectral, Thermal and Luminescent Properties of Nd3+ Doped Borophosphate Glasses for 1075 nm NIR Photonic broad band Amplification applications,IOSR Appl.Phys.18,16-27.
[2] Sailaja,P.,Mahamuda,Sk.,Dedeepya,G.,Alzahrani,J.S.,Swapna,K.,Venkateswarlu,M.,Rao,A.S.,Alrowaili,Z.A.,Olarinoye,I.O.,Al-Buriahi,M.S.(2024).Effect of Eu3+ ions concentration on visible red luminescence and radiative shielding properties of SrO-Al2O3-BaCl2-B2O3-TeO2 glasses,Rad.Phys.Chem.216,111467.
[3] Rani,P.R.,Venkateswarlu,M.,Mahamuda,S.,Swapna,K.,Deopa,N.,Rao,A.S.,Prakash,G.V.(2019).Structural,absorption and photoluminescence studies Sm3+ ions doped barium lead fluoroborate glasses for optoelectronic device applications. Mat. Reasearch Bulletin,110, 159-168.
[4] Meena,S.L.(2024).Spectral and Thermal properties of Tm3+ doped in Zinc Lithium Tungsten Alumino Phosphate glasses,IOSR Appl.Phys.16,64-75
[5] Meena,S.L.(2026).Spectral, Transmittance and Thermal Analysis of Tb3+ doped Ytterbium Zinc Lithium Calcium Borogerminate Glasses,IOSR,Appl.Phys.18,31-38.
[6] Wang,M.T.,Cheng,J.S.,Li,M.,He,F.(2011).Structure and properties of sodalime silicate glass doped with rare earth.Phys.B Condens.Matter,406,187-191.
[7] Zhao,G.Y.,Tian,Y.,Wang,X.,Fan,H.Y.,Hu,L.L.(2013).Spectroscopicproperties of 1.08µm emission in Tm3+ doped bismuth silicate glass,J.Lumin.134,837-841.
[8] Babu,K.V.,Cole,S.(2018).Luminescence properties of Dy3+ doped alkali lead alumino borosilicate glasses,Ceram.Int.9080-9090.
[9] Cao,W.,Huang,F.,Wang,T.,Ye,R.,Lei,R.,Tian,Y.,Zhang,J.,Xu,S.(2018).2.0µm emission of Ho3+ doped germanosilicate glass sensitized by non-rare earth ion Bi: a new choice for 2.0 µm laser,Opt.Mater,75,695-698.
[10] Monisha, M., Nancy,A. , Souza, D., Nimitha ,V. L., Prabhu, S and Sayyed, M.I.(2020). Dy3+ doped SiO2- B2O3-Al2O3-NaF-ZnF2 glasses: An exploration of optical and gamma radiation shielding features, Current Applied Physics 20(11), 1207-1210.
[11] Sroda,M.,Swiontek,S.,Gieszczyk,W.,Bilski,P.(2020).The effect of lithium fluoride on the thermal stability and thermoluminescence properties of borosilicate glass and glass ceramics,J.Eur,Ceram.Soc.40,472-479.
[12] Mi-tang Wang , Jin-shu Cheng, Mei Li and Feng He(2011). Structure and properties of soda lime silicate glass doped with rare earth. Physica B 406, 187–191.
[13] Tian,C.,Chen,Xi,Shuibao,Yu(2015).Concentration dependence of spectroscopic properties and energy transfer analysis in Nd3+ doped bismuth silicate glasses,Solid State Sci.48,171-176.
[14] Meena,S.L.(2021).Spectral and Raman Analysis of Sm3+ doped in Zinc Lithium Sodalime Alumino Silicate Glasses,Int.J.Eng.Sci.Inven.10,28-33.
[15] Yasukevich,A.S.,Dunia,G.,Kisel,V.E.E.,Kuleshov,N.V.(2020).Spectralluminescence properties of oxyfluoride lead silicate germinate.J.Lumin.229,117667.
[16] Meena,S.L.(2025).Spectral, Thermal and Raman Analysis of Dy3+ Doped Borosilicate Glasses with Large Thermal Stability Parameter, Int.J.Eng.Sci.Inv.14,11-18.
[17] Matos,I.M.,Balzaretti, N.M.(2024).Effect of mixed alkali ions on the structural and spectroscopic properties of Nd3+ doped silicate glasses,Res.Mat.21,100517,1-8.
[18] Meena,S.L.(2020).Judd-Ofelt analysis of Gd3+ Doped in Lead Lithium Antimony Alumino Sodalime Silicate Glasses, Int.J.Chem.Phy.Sci.9,13-22.
[19] Meena,S.L.(2021). Spectral and Thermal properties of Pr3+ doped lead lithium sodium tungsten borophosphate glasses,IOSR Appl.Phys.13,1-7.
[20] Meena,S.L.(2021). Spectral and Raman Analysis of Er3+ doped Zinc Lithium Antimony Sodalime Tellurite Glasses,Int.J.Eng.Sci.Inv.10,09-15.
[21] Judd, B.R. (1962). Optical Absorption Intensities of Rare Earth Ions. Physical Review, 127, 750.
[22] Ofelt, G.S. (1962). Intensities of Crystal Spectra of Rare Earth Ions. The J. Chem. Phys., 37, 511.
[23] Sinha, S.P. (1983). Systematics and properties of lanthanides, Reidel, Dordrecht.
[24] Krupke, W.F. (1974).IEEE J. Quantum Electron QE, 10,450.
[25] Meena,S.L.(2026). Spectral,Thermal and Luminescent properties of Nd3+ doped borophosphate glasses for 1075µm NIR Photonic broad band Amplification applications, glasses, IOSR Appl.Phys.18,16-23.
[26] Meena,S.L.(2024).Spectral and Luminescence Study of Er3+ doped Phosphate Glasses for the Development of 1.5 ?m Broadband Amplifier,IOSR Appl.Phys.16,35-41.