ETRI Journal | |
Improvement of 4I11/2 -> 4I13/2 Transition Rate and Thermal Stabilities in Er3+-Doped TeO2 | |
关键词: emission cross section; lifetime; GeO2; B2O3; tellurite glass; Er; Optical amplifier; | |
Others : 1184360 DOI : 10.4218/etrij.01.0101.0401 |
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【 摘 要 】
Spectroscopic and thermal analysis indicates that tellurite glasses doped with B2O3 and GeO2 are promising candidatehost materials for wide-band erbium doped fiber amplifier (EDFA) with a high 980 nm pump efficiency. In this study, we measured the thermal stabilities and the emission cross-sections for Er3+: 4I13/2 ? 4I15/2 transition in this tellurite glass system. We also determined the Judd-Ofelt parameters and calculated the radiative transition rates and the multipho-non relaxation rates in this glass system. The 15 mol% sub-stitution of B2O3 for TeO2 in the Er3+-doped 75TeO2-20ZnO-5K2O glass raised the multiphonon relaxation rate for 4I11/2? 4I13/2 transition from 4960 s-1 to 24700 s-1, but shortened the lifetime of the 4I13/2 level by 14 % and reduced the emis-sion cross-section for the 4I13/2 ? 4I15/2 transition by 11%. The 15 mol% GeO2 substitution in the same glass system also reduced the emission cross-section but increased the lifetime by 7%. However, the multiphonon relaxation ratefor 4I11/2? 4I13/2 transition was raised merely by 1000 s-1.Therefore, a mixed substitution of B2O3 and GeO2 for TeO2was concluded to be suitable for the 980 nm pump effi-ciency and the fluorescence efficiency of 4I13/2 ? 4I15/2 transitionin Er3+-doped tellurite glasses.
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【 预 览 】
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【 参考文献 】
- [1]A. Mori, Y. Ohishi, M. Yamada, H. Ono, Y. Nishida, K. Oikawa, and S. Sudo, "1.5 μm Broadband Amplification by Tellurite-Based EDFAs," Technical Digest of Conf. Optical Fibe-Comm.1997 (OFC’97), Feb. 16-21, 1997, Dallas, Texas, US, PD1
- [2]Y. Ohishi, A. Mori, M. Yamada, H. Ono, Y. Nishida, and K. Oi-kawa, "Gain Characteristics of Tellurite-Based Erbium-Doped Fiber Amplifiers for 1.5-μm Broadband Amplification," Opt. Lett., vol. 23, no. 4, 1998, p.274.
- [3]W.J. Miniscalco, "Erbium-Doped Glasses for Fiber Amplifiers at 1500 nm," J. Lightwave Technol., vol. 9, 1991, p.234.
- [4]T. Nakai, Y. Noda, T. Tani, Y. Mimura, T. Sudo, and S. Ohno, "980 nm-Pumped Er-Doped Tellurite-Based Fiber Amplifier," OSA TOPS, vol. 25, 1998, p.82.
- [5]M.P. Hehlen, N.J. Cockroft, T.R. Gosnell, and A.J. Bruce, "Spec-troscopic Properties of Er3+- and Yb3+-Doped Soda-Lime Silicate and Aluminosilicate Glasses," Phys. Rev. B, vol. 56, 1997, p.9302.
- [6]R. Reisfeld and C.K. Jorgensen, in Handbook of Physics and Chemistry of Rare Earths, edited by K.A. Gschneidner, Jr. and L. Eyring, Elsevier Science Publishers B.V., 1987.
- [7]X. Zou and T. Izumitani, "Spectroscopic Properties of Er3+- and Yb3+-Doped Soda-Lime Silicate and Aluminosilicate Glasses," J. Non-Cryst. Solids, vol. 162,1993, p.68.
- [8]R.S. Quimby, "Output Saturation in a 980 nm Pumped Erbium-Doped Fiber Amplifier," Appl. Opt., vol. 30, 1991, p.2546.
- [9]Y.G. Choi, D.S. Lim, K.H. Kim, D.H. Cho, and H.K. Lee, "En-hanced 4I11/2 → 4I13/2 Transition Rate in Er3+/Ce3+-Codoped Tel-lurite Glasses," Electron. Lett. vol. 35, no. 20, 1999, p.1765.
- [10]J.S. Wang, E.M. Vogel, and E. Snitzer, "Tellurite Glass: a New Candidate for Fiber Devices," Optical Materials, vol. 3, 1994, p.187.
- [11]M.G. Drexhage, O.H. El-Bayoumi, C.T. Moynihan, A.J. Bruce, K.H. Chung, D.L. Gavin, and J.T. Loretz, "Preparation and Prop-erties of Heavy-Metal Fluoride Glasses Containing Ytterbium or Lutetium," J. Am. Ceram. Soc. vol. 65, 1982, p.168.
- [12]H. Toratani, T. Izumitani, and H. Kuroda, "Compositional De-pendence of Nonradiative Decay Rate in Nd Laser Glasses," J. Non-Cryst. Solids, vol. 52, 1982, p.303.
- [13]Z. Pan and S.H. Morgan, "Optical Transitions of Er3+ in Lead-Tellurium-Germanate Glasses," J. Lumin., vol. 75, 1997, p.301.
- [14]B.R. Judd, "Optical Absorption Intensities of Rare Earth Ions," Phys. Rev., vol. 127, 1962, p.750.
- [15]G.S. Ofelt, "Intensities of Crystal Spectra of Rare Earth Ions," J. Chem. Phys., vol. 37, 1962, p.511.
- [16]M.J. Weber, "Probabilities for Radiative and Nonradiative Decay of Er3+ in LaF3," Phys. Rev., vol. 157, 1967, p.262.
- [17]M.D. Shinn, W.A. Silbley, M.G. Drexhage, and R.N. Brown, "Op-tical Transitions of Er3+ Ions in Fluorozirconate Glass," Phys. Rev. B, vol. 27, 1983, p.6635.
- [18]M.J. Weber, "Multiphonon Relaxation of Rare-Earth Ions in Yt-trium Orthoaluminate," Phys Rev. B, vol. 8, no.1, 1973, p.54.
- [19]T. Miyakawa and D.L. Dexter, "Photon Sidebands, Multiphonon Relaxation of Excited States, and Phonon-Assisted Energy Trans-fer between Ions in Solids," Phys. Rev. B, vol. 1, 1970, p.2961.
- [20]Y. Ohishi, Optical Fiber Amplifiers: Materials, Devices, and Ap-plications, edited by S. Sudo, Artech House, 1997.
- [21]A.A. Kaminski, Laser Crystals: Their Physics and Properties, Springer, Berlin, 1975.
- [22]E. Desurvire, Erbium-Doped Fiber Amplifiers: Principles and Applications, John Wiley & Sons, 1994.
- [23]K. Wei, D.P. Machewirth, J. Wenzel, E. Snitzer, and G.H. Sigel Jr., "Pr3+-Doped Ge-Ga-S Glasses for 1.3 μm Optical Fiber Amplifi-ers," J. Non-Cryst. Solids, vol. 182, 1995, p.257.
- [24]D.E. Mc Cumber, "Theory of Phonon-Terminated Optical Ma-sers," Phys. Rev. A, vol. 134, 1964, p.299.
- [25]W.J. Miniscalco and R.S. Quimby, "General Procedure for the Analysis of Er3+ Cross-Sections," Opt. Lett., vol. 16, 1991, p.258.
- [26]R. Reisfeld and C.K. Jorgensen, Laser and Excited States of Rare Earths, Springer-Verlag, New York, 1997.
- [27]D.R. Simons, A.J. Faber, and H. de Waal, "Pr3+-Doped GeSx-Based Glasses for Fiber Amplifiers at 1.3 μm," Opt. Lett., vol. 20, no. 5, 1995, p. 468.
- [28]Yong Gyu Choi, Bong Je Park, Kyong Hon Kim, and Jong Heo, "Pr3+- and Pr3+/Er3+-Doped Selenide Glasses for Potential 1.6 μm Optical Amplifier Materials," ETRI J., vol. 23, no. 3, 2001, p. 97.