Glass sample of Zinc Lithium Tungsten Sodalime Borotellurite: (35-x) TeO2:10ZnO:10Li2O:10WO3:10CaO:10Na2O:15B2O3:xTm2O3. (where x=1,1.5 and 2 mol%) have been prepared by melt-quenching technique.
The amorphous nature of the prepared glass samples was confirmed by X-ray diffraction. Optical absorption ,fluorescence and FTIR spectra were recorded at room temperature for all glass samples. Judd-Ofelt intensity parameters ?? (?=2, 4 and 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
I. INTRODUCTION
Transparent glass–ceramic as host materials for active optical ions have attracted great interest recently due to their potential application in optical devices such as frequency-conversion materials, lasers and optical fiber amplifiers [1-5]. Among these hosts, the borotellutite system is attractive due to its superior physical, structural and optical properties [6, 7]. ZnO is a wide band gap semiconductor and has received increasing research interest. It is an important multifunctional material due to its specific chemical, surface and micro structural properties [8]. Tellurite glasses have a low glass transition temperature, low melting temperature and high gain density.
The high gain density in tellurite glasses is due to high solubility of rare earth ions in tellurite network [9-14]. Recently, glass-ceramics containing dysprosium oxides have been found in applications for several different purposes. Tm3+ doped glasses have attracted much interest due to their important optical properties used in lasers, optical amplifiers, network formers, photonic devices and as infrared sensors [15-18].
The present work reports on the preparation and characterization of rare earth doped heavy metal oxide (HMO) glass systems for lasing materials. I have studied on the absorption, emission and FTIR properties of Tm3+ doped zinc lithium tungsten sodalime borotellurite glasses.
The intensities of the transitions for the rare earth ions have been estimated successfully using the Judd-Ofelt theory, The laser parameters such as radiative probabilities(A),branching ratio (β), radiative life time(τR) and stimulated emission cross section(σp) are evaluated using J.O.intensity parameters( Ωλ, λ=2,4 and 6).
II. EXPERIMENTAL TECHNIQUES
A. Preparation of Glasses
The following Tm3+doped borotellurite glass samples (35-x) TeO2:10ZnO:10Li2O:10WO3:10CaO:10Na2O:15B2O3:xTm2O3. (where x=1,1.5 and 2 mol%) have been prepared by melt-quenching method. Analytical reagent grade chemical used in the present study consist of TeO2, ZnO, Li2O, WO3, CaO, Na2O3,B2O3 and Tm2O3.
They were thoroughly mixed by using an agate pestle mortar. then melted at 9800C by an electrical muffle furnace for 2h., After complete melting, the melts were quickly poured in to a preheated stainless steel mould and annealed at temperature of 2500C for 2h to remove thermal strains and stresses. Every time fine powder of cerium oxide was used for polishing the samples. The glass samples so prepared were of good optical quality and were transparent. The chemical compositions of the glasses with the name of samples are summarized in Table 1.
Conclusion
In the present study, the glass samples of composition (35-x)TeO2:10ZnO:10Li2O:10WO3:10CaO:10Na2O:15B2O3
:xTm2O3. (where x =1, 1.5 and 2mol %) have been prepared by melt-quenching method. The value of stimulated emission cross-section (?p) is found to be maximum for the transition (3F4?3H6) for glass ZLTSLBT (TM 01), suggesting that glass ZLTSLBT (TM 01) is better compared to the other two glass systems ZLTSLBT (TM 1.5) and ZLTSLBT (TM 02).
References
[1] Zhang ,X.,Hu,L. and Ren,J. (2020). Structural Studies of Rare Earth-Doped Fluoroborosilicate Glasses by Advanced Solid-State NMR, . Phys.Chem.123(16),8919-8929.
[2] Liyu Hao, Manting Pei, Tie Yang, Chengguo Ming(2020).Double sensitivity temperature sensor based on excitation intensity ratio of Eu3+ doped phosphate glass ceramic, Optik 204,164188.
[3] Areej, S. Alqarni, R., Hussin, S.N., Alamri and Ghoshal, S.K.(2020).Tailored structures and dielectric traits of holmium ion-doped zinc-sulpho-boro-phosphate glass ceramics, Ceremics International 46(3),3282-3291.
[4] Haijian Li, Jianhua Yi, Zhao Qin, Zhihua Sun, Yi Xu, Changjian Wang, Fengqi Zhao, Yucheng Hao and Xiaofeng L., (2019). Structures, Thermal expansion, chemical stability and crystallization behavior of phosphate based glasses by influence of rare earth, Journal of Non- Crystalline Sollids 522,119602.
[5] Mikko Hongisto, Alxender Vebar, Nadia Giovanna, S. Danto, Veronique and L. Petit(2020).Transparent Yb3+ doped phosphate glass ceramics, Ceremics International 46(16),26317-26325.
[6] Elkhoshkhany,N., Khatab, M.A. and Kabary, M.A.(2018).Thermal, FTIR and UV spectral studies on tellurite glasses doped with cerium oxide,Ceram Int, 44 , 2789-2796.
[7] Wagh, A., Raviprakash,Y., Upadhyaya, V. and Kamath, S.D.(2015).Composition dependent structural and optical properties of PbF2–TeO2–B2O3–Eu2O3 glasses, Spectrochim Acta A Mol Biomol Spectrosc, 151, 696-706
[8] Pavani, P. G., Sadhana, K. and Mouli, V. C. (2011).Optical, physical and structural studies of boro-zinc tellurite glasses, Physica B: Condensed Matter, 406, 7, 1247.
[9] P.Nandi and G.Jose (2006). Spectroscopic Properties of Er3+ Doped Phospho-Tellurite Glasses,Physica B Condensed Matter,381(1),66-72.
[10] Anashkina, E.A.(2020).Laser Sources Based on Rare-Earth Ion Doped Tellurite Glass Fibers and Microspheres, Fibers , 8,1-17.
[11] Jha, A., Richards, B., Jose, G., Teddy-Fernandez, T., Joshi, P.m, Jiang, X. and Lousteau(2012).J. Rare-earth ion doped TeO2 and GeO2 glasses as laser materials. Prog. Mater. Sci., 57, 1426–1491
[12] Kishi, T., Kumagai, T., Shibuya, S., Prudenzano, F., Yano, T. and Shibata, S.(2015). Quasi-single mode laser output from a terrace structure added on Nd 3+-doped tellurite-glass microsphere prepared using localized laser heating. Opt. Express, 23, 20629–20635.
[13] Anashkina, E. A.(2020). Laser Sources Based on Rare-Earth Ion Doped Tellurite Glass Fibers and Microspheres, Fibers , 8 (30),1-17.
[14] Qin, J., Huang, Y., Liao, T., Xu, C., Ke, C. and Duan, Y.(2019). 1.9 µm laser and visible light emissions in Er3+/Tm3+ co-doped tellurite glass microspheres pumped by a broadband amplified spontaneous emission source. J. Opt., 21, 035401.
[15] Lachheb, R., Damak, K., Assadi, A.A., Herrmann, A., Yousef, E., Rüssel, C.and Maâlej, R.(2015). Characterization of Tm3+ doped TNZL glass laser material. J. Lumin., 161, 281–287.
[16] Lalla, E.A., Konstantinidis, M., De Souza, I., Daly, M.G., Martín, I.R., Lavín, V. and Rodríguez-Mendoza, U.R.(2020). Judd-Ofelt parameters of RE3+-doped fluorotellurite glass (RE3+ = Pr3+, Nd3+, Sm3+, Tb3+, Dy3+, Ho3+, Er3+, and Tm3+). J. Alloys Compd., 845, 156028.
[17] El-Maaref, A.A., Wahab, E. A., Shaaban, Kh S., Abdelawwad, M., Koubisy, M. S., Boercsoek, J.and Sayed Yousef, El (2020).Visible and mid-infrared spectral emissions and radiative rates calculations of Tm3+ doped BBLC glass, Spectrochimica Acta Part A- Molecular and Biomolecular Spectroscopy, 242, 118774.
[18] Sharma, R., Prasad, A., Kaur, S., Deopa,N., Rani, R., Venkateswarlu, M.and Rao, A.S.(2019). Spectroscopic properties of deep red emitting Tm3+ doped ZnPbWTe glasses for optoelectronic and laser applications, Journal of NonCrystalline Solids. 516, 82–88.
[19] Gorller-Walrand, C. and Binnemans, K. (1988). Spectral Intensities of f-f Transition. In: Gshneidner Jr., K.A. and Eyring, L., Eds., Handbook on the Physics and Chemistry of Rare Earths, Vol. 25, Chap. 167, North-Holland, Amsterdam, 101.
[20] Sharma, Y.K., Surana, S.S.L. and Singh, R.K. (2009). Spectroscopic Investigations and Luminescence Spectra of Sm3+ Doped Soda Lime Silicate Glasses. Journal of Rare Earths, 27, 773.
[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 Journal of Chemical Physics, 37, 511.
[23] Elkhoshkhany,N., Marzouk, S. Y., Khattab, M. A.and Dessouki, S. A.(2018). Influence of Sm2O3 addition on JuddOfelt parameters, thermal and optical properties of the TeO2-Li2O-ZnO-Nb2O5 glass system, Mater. Charact. 144 274–286.
[24] Elkhoshkhany, N.and Mohamed, H.M.(2019). UV–Vis-NIR spectroscopy, structural and thermal properties of novel oxyhalide tellurite glasses with composition TeO2 -B2O3 -SrCl2 -LiF-Bi2O3 for optical application. Res. Phys., 13, 102222.
[25] Mansour, E.(2012). FTIR spectra of pseudo-binary sodium borate glasses containing TeO2, J. Mol. Struct. 1014, 1–6.