制备了碲酸盐玻璃样品70TeO2-(15-x)B2O3-xNb2O5-15ZnO-1wt%Er2O3(TBN,x=0,3,6,9,12,15 mol%).测试了玻璃样品的热稳定性和光谱性质.根据Judd-Ofelt理论计算了TBN玻璃中Er3+离子的强度参数(Ω2=(5.42~6.76)×10-20 cm2,Ω4=(1.37~1.73)×10-20cm2,Ω6=(0.70~0.94)×10-20 cm2),发现随着Nb2O5含量的增加,Ωt(t=2,4,6)先增加后减小.研究表明Er-O键共价性主要受基质玻璃中非桥氧数的影响,而阴阳离子间电负性的影响可以忽略.应用McCumber理论计算了Er3+离子的受激发射截面(σe=(0.77~0.91)×10-20 cm2)和Er3+离子4I13/2→4I15/2发射谱的半高宽度(FWHM=65~73 nm).比较了不同基质玻璃中Er3+离子的荧光半高宽和受激发射截面.结果表明TBN玻璃系统具有较好的带宽性能,是一种制备宽带光纤放大器的潜在基质材料.
参考文献
[1] | Yang J H,Dai S X,Dai N L,et al.Effect of Bi2O3 on the spectroscopic properties of erbium-doped bismuth silicate glasses[J].J.Opt.Soc.Am.B,2003,20(5):810-815. |
[2] | Sun J T,Zhang J H,Luo Y S,et al.Spectra and its bandwidth of the 1.5 μm emission in Er3+-doped glass[J].J.Optoelectronics Laser,2003,14(9):992-995. |
[3] | Neindre L L,Jiang S B,Hwang B C,et al.Effect of relative alkali content on absorption linewidth in erbium-doped tellurite glass[J].J.Non-Cryst.Solids,1999,255:97-102. |
[4] | Wang J S,Vogel E M,Snitzer E,et al.Tellurite glass:A new candidate for fiber devices[J].J.Opt.Mater,1994,3(4):187-203. |
[5] | Feng X,Tanabe Setsuhisa,Hanada Teiichi.Spectroscopic properties and thermal stability of Er3+-doped germanotellurite glasses for broadband fiber amplifiers[J].J.Am.Ceram.Soc,2001,84 (1):165-171. |
[6] | Chen B Y,Chen D D,Liu Y H,et al.Effect of mixed alkali on the thermal stability of tellurite glasses[J].J.South China University of Technology (Natural Science Edition),2004,32(4):48-51. |
[7] | Judd B R.Optical absorption intensities of rare-earth ions[J].J.Phys.Rev.,1962,127(3):750-761. |
[8] | Ofelt G S.Intensities of crystal spectra of rare-earth ions[J].J.Chem.Phys.,1962,37(3):511-520. |
[9] | Ebendorff-Heidepriem H,Ehrt D,Bettinelli M,et al.Effect of glass composition on Judd-Ofelt parameters and radiative decay rates of Er3+ in fluoride phosphate and phosphate glasses[J].J.Non-Cryst.Solids,1998,240(1-3):66-78. |
[10] | Tanabe S.Optical transitions of rare earth ions for amplifiers:How the local structure works in glass[J].J.Non-Cryst.Solids,1999,259(1-3):1-9. |
[11] | Lin J,Huang W H,Zhu X R,et al.The impact of ZnO on structure and optical performance for TeO2-Nb2O5glass[J].J.Function Materials,2003,34(6):711-713. |
[12] | Pauling L.The Nature of the Chemical Bond[M].Third edition.Ithaca:Cornell University Press,N.Y.1960. |
[13] | Cowan R D.The Theory of Atomic Structure and Spectra[M].Berkeley:University of California Press,1981. |
[14] | Lin H,Pun E,Man S Q,et al.Optical transitions and frequency upconversion of Er3+ ions in Na2O-Ca3Al2Ge3O12glass[J].J.Opt.Soc.Am.B,2001,18(5):602-609. |
[15] | Zou X L,Izumitani T.Spectroscopic properties and mechanisms of excited state absorption and energy transfer upconversion for Er3+-doped glasses[J].J.Non-Cryst.Solids,1993,162(1-2):68-80. |
[16] | Righini G C,Pelli S,Fossi M,et al.Characterization of Er-doped sodium-niobium phosphate glasses[C]//Proc.SPIE,2001,4282:210-215. |
[17] | Tanabe S,Sugimoto N,Hanada T,et al.Broadband 1.5um emission of Er3+ irons in bismuth-based oxide glasses for potential WDM amplifier[J].J.Lumin,2000,87-89:670-672. |
[18] | McCumber D E.Theory of phonon-terminated optical masers[J].J.Phys.Rev.,1964,134(2A):A299-A306. |
[19] | Jiang S B,Luo T,Hwang Bor-Chyuan,et al.Er3+-doped phosphate glasses for fiber amplifiers with high gain per unit length[J].J.Non-Cryst.Solids,2002,263-264:364-368. |
[20] | Tanabe S,Yoshii S,Hirao K,et al.Upconversion properties,multiphonon relaxation and local environment of rare-earth ions in fluorophosphates glasses[J].J.Phys.Rev.B,1992,45(9):4620-4625. |
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