Sm3+ Doped Lithium Strontium Borate Glasses for Solid State Lighting Applications
- Authors: Venugopal A.R.1,2,3, Rajaramakrishna R.4,5, Abhiram J.4, Pattar V.2, Rajashekara K.M.1, Kaewkhao J.5
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Affiliations:
- Department of Physic, B.G.S R&D Centre, SJC Institute of Technology
- Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR)
- Department of Physics, Brindavan College of Engineering
- Department of PG Studies and Research in Physics, The National College
- Center of Excellence in Glass Technology and Materials Science (CEGM), Nakhon Pathom Rajabhat University
- Issue: Vol 45, No 6 (2019)
- Pages: 472-484
- Section: Article
- URL: https://journals.rcsi.science/1087-6596/article/view/217438
- DOI: https://doi.org/10.1134/S1087659620010216
- ID: 217438
Cite item
Abstract
The glasses of samarium (0.1, 0.2, 0.5, 1.0, 1.5 and 2.0 mol %) doped lithium strontium borate samples were synthesized. The physical and optical properties are studied at ambient conditions and discussed in this study. XRD spectra reveals the no atomic order in structure (amorphous) present in these glasses. Infrared spectroscopic study reveals the structural units of borate viz., BO3 and BO4 group present in the matrix. Interestingly, it is found that as the rare earth concentration increases and beyond 1.5 mol % the luminescence intensity decreases due to non-bridging Sm3+ ions in the glass network. The peaks in absorption spectra are due to dipole transition from 6H5/2 to levels corresponds to (2S + 1)LJ excited states under the excitation wavelength of 402 nm. Judd–Ofelt theory applied to estimate dipole strength in terms of J–O parameters (Ω2, Ω4 and Ω6), oscillator strength (fexp and fcal), radiative transition possibility (AR), branching ratio (βR) and stimulated emission cross section (σ) of the glass samples. From Judd–Ofelt analysis the parameters obtained are shown for 1.50 mol % of Sm3+ doped lithium strontium borate (LSB) glasses studied, which were compared with other glasses. The obtained results suggest their potential candidature for using as solid state material lighting applications due their efficient orange emissions.
About the authors
A. R. Venugopal
Department of Physic, B.G.S R&D Centre, SJC Institute of Technology; Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR); Department of Physics, Brindavan College of Engineering
Email: r.rajaramakrishna@gmail.com
India, Chikkaballapur, Karnataka; JalahalliBengaluru, Jakkur, 560064; Bengaluru, 560063
R. Rajaramakrishna
Department of PG Studies and Research in Physics, The National College; Center of Excellence in Glass Technology and Materials Science (CEGM), Nakhon Pathom Rajabhat University
Author for correspondence.
Email: r.rajaramakrishna@gmail.com
India, JayanagarBangalore, 560070; Nakhon Pathom, 73000
J. Abhiram
Department of PG Studies and Research in Physics, The National College
Email: r.rajaramakrishna@gmail.com
India, JayanagarBangalore, 560070
Vinayak Pattar
Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR)
Email: r.rajaramakrishna@gmail.com
India, JalahalliBengaluru, Jakkur, 560064
K. M. Rajashekara
Department of Physic, B.G.S R&D Centre, SJC Institute of Technology
Email: r.rajaramakrishna@gmail.com
India, Chikkaballapur, Karnataka
J. Kaewkhao
Center of Excellence in Glass Technology and Materials Science (CEGM), Nakhon Pathom Rajabhat University
Email: r.rajaramakrishna@gmail.com
Thailand, Nakhon Pathom, 73000
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