Hypersensitivity and nephelauxetic effect of Er3+ in bismuth tellurite glass system

Results in Chemistry - Tập 6 - Trang 101085 - 2023
M.S. Sutrisno1,2, N.N. Yusof3, M.N. Azlan4, M.H.M. Zaid5, S.M. Iskandar3, R. Hisam1
1Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia
2University of Cyberjaya (UoC), Persiaran Bestari, Cyber 11, 63000 Cyberjaya, Selangor, Malaysia
3School of Physics, Universiti Sains Malaysia, 11800 USM Penang, Malaysia
4Physics Department, Faculty of Science and Mathematics, Universiti Pendidikan Sultan Idris, 35900 Tanjong Malim, Perak, Malaysia
5Department of Physics, Faculty of Science, Universiti Putra Malaysia, 43400, Serdang, Selangor, Malaysia

Tài liệu tham khảo

Jamalaiah, 2012, Visible and near infrared luminescence properties of Er3+ doped LBTAF glasses for optical amplifiers, Optical Mater., 34, 861, 10.1016/j.optmat.2011.11.023 Ramachari, 2014, Gain properties and concentration quenching of Er3+ doped niobium oxyfluorosilicate glasses for photonic applications, Opt. Mater., 36, 823, 10.1016/j.optmat.2013.12.013 Selvaraju, 2013, Composition dependent spectroscopic properties of Er3+ doped boro-tellurite glasses, physica status solidi (a), 210, 607, 10.1002/pssa.201228191 Huang, 2001, Stark levels analysis for Er3+ doped oxide glasses: germanate and silicate, Opt. Mater., 15, 243, 10.1016/S0925-3467(00)00039-2 Gruber, 1993, Energy levels and correlation crystal-field effects in Er3+ doped garnets, Phys. Rev. B, 48, 15561, 10.1103/PhysRevB.48.15561 Lüthi, 1998, Electronic energy-level structure, correlation crystal-field effects, and f− f transition intensities of Er3+ in Cs3Lu2Cl9, Phys. Rev. B, 57, 15229, 10.1103/PhysRevB.57.15229 Hehlen, 2013, 50th anniversary of the Judd-Ofelt theory: An experimentalist's view of the formalism and its application, J. Lumin., 136, 221, 10.1016/j.jlumin.2012.10.035 Babu, 2012, Spectral studies of Erbium doped heavy metal borophosphate glass systems, Phys. B Condens. Matter, 407, 705, 10.1016/j.physb.2011.12.006 Arunkumar, 2015, Spectroscopic properties of Er3+ doped bismuth lead telluroborate glasses for 1.53 μm optical amplifiers, J. Alloy. Compd., 627, 54, 10.1016/j.jallcom.2014.12.016 Jørgensen, 1962, The nephelauxetic series, Prog. Inorg. Chem., 73 Wensky, D. A., & Moulton, W. G. (1970). Energy levels of Pr3+ in various crystal hosts.The Journal of Chemical Physics,53(10), 3957-3969. Sovers, O. J., & Yoshioka, T. (1969). Host cation effects on the fluorescence spectrum of Eu3+ in oxysulfides.The journal of chemical physics,51(12), 5330-5336. Tanner, 2013, Nephelauxetic effects in the electronic spectra of Pr3+, Chem. A Eur. J., 117, 10726 Tandon, 1969, Bonding Inferred from Study of Nephelauxetic Effect in Praseodymium Complexes, Spectrosc. Lett., 2, 255, 10.1080/00387016908050051 Petit, 2006, A theoretical characterization of covalency in rare earth complexes through their absorption electronic properties: f− f transitions, Inorg. Chem., 45, 7382, 10.1021/ic060149x Morrison, 1967, Modified slater integrals for an ion in a solid, Phys. Lett. A, 24, 607, 10.1016/0375-9601(67)90642-1 Angelov, 1984, Nephelauxetic effect and (rk) 4f expectation values of Er3+ in ionic crystals, J. Phys. C Solid State Phys., 17, 1709, 10.1088/0022-3719/17/10/013 Newman, 1973, Slater parameter shifts in substituted lanthanide ions, J. Phys. Chem. Solid, 34, 541, 10.1016/0022-3697(73)90049-8 Henrie, 1976, Hypersensitivity in the electronic transitions of lanthanide and actinide complexes, Coord. Chem. Rev., 18, 199, 10.1016/S0010-8545(00)82044-5 Görller-Walrand, 1998, Spectral intensities of f-f transitions, Handb. Phys. Chem. Rare Earths, 25, 101, 10.1016/S0168-1273(98)25006-9 Peacock, 1977, The charge-transfer contribution to the intensity of hypersensitive trivalent lanthanide transitions, Mol. Phys., 33, 1239, 10.1080/00268977700101051 Iftikhar, 1987, Hypersensitivity in the 4f–4f absorption spectra of lanthanide (III) complexes, Inorg. Chim. Acta, 129, 261, 10.1016/S0020-1693(00)86672-4 Devi, 1996, Optical properties of Er3+ ions in lithium borate glasses and comparative energy level analyses of Er3+ ions in various glasses, J. Non Cryst. Solids, 197, 111, 10.1016/0022-3093(95)00573-0 Lakshman, 1980, Racah and Judd-Ofelt parameters for Pr3+, Nd3+, and Er3+ ions in a laser liquid, J. Quant. Spectrosc. Radiat. Transf., 24, 251, 10.1016/0022-4073(80)90067-9 Yeung, 2015, Trends in atomic parameters for crystals and free ions across the lanthanide series: the case of LaCl3: Ln3+, Chem. A Eur. J., 119, 6309 Mortier, 2000, Crystal field analysis of Er3+ doped glasses: germanate, silicate and ZBLAN, J. Alloy. Compd., 300, 407, 10.1016/S0925-8388(99)00753-7 Kaewwiset, 2013, ESR and spectral studies of Er3+ ions in soda-lime silicate glass, Phys. B Condens. Matter, 409, 24, 10.1016/j.physb.2012.10.004 Carnall, 1965, Spectral intensities of the trivalent lanthanides and actinides in solution. I. Pr3+, Nd3+, Er3+, Tm3+, and Yb3+, J. Chem. Phys., 42, 3797, 10.1063/1.1695840 Auzel, 1983, A scalar crystal field strength parameter for rare-earth ions: meaning and usefulness, J. Phys., 44, 201, 10.1051/jphys:01983004402020100 Gatterer, 1994, Hypersensitivity and nephelauxetic effect of Nd (III) in sodium borate glasses, J. Non Cryst. Solids, 176, 237, 10.1016/0022-3093(94)90082-5 Sutrisno, 2022, DC conductivity, optical properties and Judd-Ofelt evaluation of 20Li2O-xBi2O3-(78–x) TeO2-1Er2O3-1Ag mixed ionic-electronic glasses, Mater. Today Commun., 31, 103525, 10.1016/j.mtcomm.2022.103525 Marcantonatos, 1986, Multiphonon non-radiative relaxation rates and Judd–Ofelt parameters of lanthanide ions in various solid hosts, J. Chem. Soc., Faraday Trans. 2, 82, 381, 10.1039/F29868200381 Sutrisno, 2022, Tailoring multiphonon relaxation and cross relaxation energy transfer in mixed ionic-electronic 20Li2O-xBi2O3-(78–x) TeO2-1Er2O3-1Ag glasses at NIR region, J. Non Cryst. Solids, 594, 121826, 10.1016/j.jnoncrysol.2022.121826 Van Dijk, J. M. F., & Schuurmans, M. F. H. (1983). On the nonradiative and radiative decay rates and a modified exponential energy gap law for 4 f–4 f transitions in rare‐earth ions.The Journal of Chemical Physics,78(9), 5317-5323. Schuurmans, 1984, On radiative and non-radiative decay times in the weak coupling limit, Physica B+ C, 123, 131, 10.1016/0378-4363(84)90117-7 Judd, 1962, Optical absorption intensities of rare-earth ions, Phys. Rev., 127, 750, 10.1103/PhysRev.127.750 Ofelt, G. S. (1962). Intensities of crystal spectra of rare‐earth ions.The journal of chemical physics,37(3), 511-520. Reisfeld, 1972, Ce3+ as a Probe of the Crystal Field and the Nature of the Impurity-Ligand Bond in Borate and Phosphate Glasses, Chem. Phys. Lett., 17, 248, 10.1016/0009-2614(72)87066-0 Reisfeld, 1975, Radiative and non-radiative transitions of rare-earth ions in glasses, 123, 10.1007/BFb0116557 Jørgensen, 1983, Judd-Ofelt parameters and chemical bonding, Journal of the Less Common Metals, 93, 107, 10.1016/0022-5088(83)90454-X Sutrisno, 2021, Effects of Bi2O3 on DC conductivity and nonlinear optical properties of mixed ionic–electronic 98 [20Li2O-xBi2O3-(80–x) TeO2]-2Ag glass system, Appl. Phys. A, 127, 1, 10.1007/s00339-021-04914-x Morrison, 1980, Host dependence of the rare-earth ion energy separation 4 f N–4fN− 1 nl, J. Chem. Phys., 72, 1001, 10.1063/1.439265 Petrov, 2014, Radial integrals< rk> 4f and nephelauxetic effect of Nd3+ in crystals, Spectrochim. Acta A Mol. Biomol. Spectrosc., 118, 199, 10.1016/j.saa.2013.08.108 Lalla, 2020, Judd-Ofelt parameters of RE3+-doped fluorotellurite glass (RE3+= Pr3+, Nd3+, Sm3+, Tb3+, Dy3+, Ho3+, Er3+, and Tm3+), J. Alloy. Compd., 845, 156028, 10.1016/j.jallcom.2020.156028 Som, 2011, Nephelauxetic effect of low phonon antimony oxide glass in absorption and photoluminescence of rare-earth ions, Spectrochim. Acta A Mol. Biomol. Spectrosc., 79, 1766, 10.1016/j.saa.2011.05.054 Tanabe, 1992, Compositional dependence of Judd-Ofelt parameters of Er3+ ions in alkali-metal borate glasses, Phys. Rev. B, 46, 3305, 10.1103/PhysRevB.46.3305 Walsh, 2006, Judd-Ofelt theory: principles and practices, 403 Richardson, 1982, On the calculation of electric dipole strengths of 4f–4f transitions in lanthanide complexes, Chem. Phys. Lett., 86, 47, 10.1016/0009-2614(82)83114-X Mahraz, 2017, Reduction of non-radiative decay rates in boro-tellurite glass via silver nanoparticles assisted surface plasmon impingement: Judd Ofelt analysis, J. Lumin., 190, 335, 10.1016/j.jlumin.2017.05.059 Saisudha, 1996, Effect of host glass on the optical absorption properties of Nd3+, Sm3+, and Dy3+ in lead borate glasses, Phys. Rev. B, 53, 6186, 10.1103/PhysRevB.53.6186 Wang, 2017, Influence of SiO2 on the Stark splitting and spectroscopic properties of Yb3+ in phosphate glass, J. Lumin., 186, 268, 10.1016/j.jlumin.2017.02.050 Cao, Y., Chen, S., Shao, C., & Yu, C. (2018). Influence of F– on stark splitting of Yb3+ and the thermal expansion of silica glass.Journal of Applied Physics,123(21), 215106. Yan, 2019, Effect of GeO2 on structure and properties of Yb: Phosphate glass, J. Non Cryst. Solids, 520, 119455, 10.1016/j.jnoncrysol.2019.05.031 Galakhov, 1973, Causes of phase separation in simple silicate systems, 7 Sun, 2020, Compositional dependence of Stark splitting and spectroscopic properties in Yb3+ doped lead silicate glasses, J. Non Cryst. Solids, 532, 119890, 10.1016/j.jnoncrysol.2020.119890