研究论文

Ho3+掺杂Ge-Ga-S-CsI玻璃中红外发光性能研究

展开
  • 1. 宁波大学 信息科学与工程学院, 宁波 315211; 2. 中国科学院 西安光学精密机械研究所 瞬态光学与光子技术国家重点实验室, 西安 710119; 3. 法国雷恩I大学 玻璃与陶瓷国家实验室, 法国 雷恩 35042

收稿日期: 2009-08-26

  修回日期: 2009-10-23

  网络出版日期: 2010-05-12

Mid-infrared Emission Properties of Ho3+-doped Ge-Ga-S-CsI Glasses

Expand
  • 1. College of Information Science and Engineering, Ningbo University, Ningbo 315211, China; 2. State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Science, Xi’an 710119, China; 3. Laboratoire de Verres et Ceramiques, Université de Rennes I, Rennes, France 35042

Received date: 2009-08-26

  Revised date: 2009-10-23

  Online published: 2010-05-12

摘要

采用熔融冷却法制备了系列不同Ho3+离子掺杂浓度的Ge-Ga-S-CsI玻璃样品,测试了样品的折射率、吸收光谱以及中红外荧光光谱和Ho3+离子5I6能级荧光寿命.应用Judd-Ofelt理论计算了Ho3+离子在该基质玻璃中强度参数Ωii=2,4,6)、能级跃迁振子强度fcal、自发跃迁几率Arad等光谱参数.计算了Ho3+5I55I6 (3.86μm)和5I65I7 (2.81μm)跃迁的多声子驰豫速率.讨论了中红外荧光特性与Ho3+离子掺杂浓度之间的关系.结果表明,在900nm 激光泵浦下观察到了2.81和3.86μm两处中红外荧光,分别对应于Ho3+5I65I75I55I6 跃迁,当Ho3+离子掺杂浓度从0.5wt%增加到1.0wt%时,两处中红外荧光强度都随相应增加,计算的Ho3+5I55I65I65I7 跃迁多声子驰豫速率分别为29s-1和34s-1.

本文引用格式

朱 军1, 戴世勋1,2, 彭 波2, 徐铁峰1, 王训四1, 章向华1,3 . Ho3+掺杂Ge-Ga-S-CsI玻璃中红外发光性能研究[J]. 无机材料学报, 2010 , 25(5) : 546 -550 . DOI: 10.3724/SP.J.1077.2010.00546

Abstract

A serial of chalcogenide glasses based on Ge-Ga-S-CsI system doped with the different Ho3+ ions were synthesized by meltquenching technique. The properties of glasses including refractive indexes, absorption spectra, midinfrared emission spectra and lifetimes of 5I6 level of Ho3+ ions were measured. The Judd Ofelt intensity parameters Ωi (i=2,4,6), oscillator strength fcal, spontaneous transition probabilities Arad for Ho3+ ion were calculated by Judd-Ofelt theory. Multiphonon relaxation rates of the Ho3+5I55I6  and 5I65I7 in Ge-Ga-S-CsI glasses were evaluated. Effect of Ho3+ ion concentration on the fluorescence spectra was investigated. The results indicate that the fluorescence under 900 nm excitation with peak wavelength at 2.81μm and 3.86μm are due to

the Ho3+5I55I6 and 5I65I7 transition, respectively. The intensity of the mid-infrared fluorescence are enhanced with the Ho3+ ion concentration increasing from 0.5wt% to 1.0wt%. Multiphonon relaxation rates are 29s-1 and 34s-1 for the Ho3+5I55I6 and 5I65I7  transition, respectively.

参考文献

[1]Sorokina I T, Vodopyanov K L. Solid-State Mid-Infrared Laser Sources. New York:Springer, 2003:219-255.
[2]Aggarwal I D, Shaw L B, Sanghera J. Chalcogenide Glass for Midand Longwave IR Fiber Lasers. SPIE, Washington, 2005:242-245.
[3]Moizan V, Nazabal V, Troles J, et al. Er3+-doped GeGaSbS glasses for midIR fibre laser application: synthesis and rare earth spectroscopy.Opt. Mater,2008, 31(1):39-46
[4]Aggarwal I D, Sanghera J S. Development and applications of chalcogenide glass optical fibers at NRL. J. Optoelectron. Adv. Mater., 2002, 4(3):665-678.
[5]Peng B, Fan Z C, Qiu X M, et al. A novel transparent vanadate glass for use in fiber optics.Adv. Mater,2005, 17(7):857-859
[6]Prudenzano F, Mescia L, Allegretti L A, et al. Design of Er3+-doped chalcogenide glass laser for MID-IR application.J. Non-Cryst. Solids,2009, 355(18-21):1145-1148
[7]Nemec P, Frumar M. Compositional dependence of spectroscopic parameters of Dy3+ ions in Ge-Ga-Se glasses.Mater. Lett,2008, 62(17/18):2799-2801
[8]Oswald J, Kuldova K, Frumarova B, et al. Near and mid-infrared luminescence of new chalcohalide glasses doped with Pr3+ ions.Mater. Sci. Eng., B,2008, 146(1/2/3):107-109
[9]Choi Y G, Song J H. Spectroscopic properties of Tm3+ ions in chalcogenide Ge-As-S glass containing minute amount of Ga and CsBr.Opt. Commun,2008, 281(17):4358-4362
[10]Lee T H, Choi Y G, Heo J. Local structure and its effect on the oscillator strengths and emission properties of Ho3+ in chalcohalide glasses.J. Non-Cryst. Solids,2008, 354(27):3107-3112
[11]Schweizer T, Samson B N, Hector J R, et al. Infrared emission from holmium doped gallium lanthanum sulphide glass.Infrared Phys. Technol,1999, 40(4):329-335
[12]Lee T H, Heo J, Choi Y G, et al. Optimized combination of Ho3+ and sulfide glass for U-band fiber-optic amplifiers.Chem. Phys. Lett,2004, 384(1/2/3):16-19
[13]Balda R, Mendioroz A, Fernandez J, et al. Laser spectroscopy and upconversion studies of Pr3+-doped halide modified sulfide glasses.Opt. Mater,2001, 16(1/2):249-254
[14]Judd B R. Optical absorption intensities of rare-earth ions.Phys. Rev,1962, 127(3):750-761
[15]Ofelt G S. Intensities of crystal spectra of rare-earth Ions.J. Chem. Phys,1962, 37(3):511-520
[16]Weber M J, Matsinger B H, Donlan V L, et al. Optical transition probabilities for trivalent holmium in LaF3 and YAlO3.J. Chem. Phys,1972, 57(1):562-567
[17]Shin Y B, Jang J N, Heo J. Mid-infrared light emission characteristics of Ho3+-doped chalcogenide and heavymetal oxide glasses.Opt. Quantum Electron,1995, 27(5):379-386
[18]Lin H, Pun E Y B, Lin X R. Er3+-doped Na2O·Cd3Al2Si3O12 glass for infrared and upconversion applications.J. Non-Cryst. Solids,2001, 283(1/2/3):27-33
[19]Peng B, Izumitani T. Optical properties, fluorescence mechanisms and energy transfer in Tm3+, Ho3+ and Tm3+ Ho3+ doped near-infrared laser glasses, sensitized by Yb3+.Opt. Mater,1995, 4(6):797-810
[20]Wetenkamp L, West G F, Tobben H. Optical properties of rare earth-doped ZBLAN glasses.J. Non-Cryst. Solids,1992, 140(7):35-40
[21]Reisfeld R, Hormadaly J. Optical intensities of holmium in tellurite, calibo, and phosphate glasses.J. Chem. Phys,1976, 64(8):3207-3212
[22]Miyakawa T, Dexter D L. Phonon sidebands, multiphonon relaxation of excited states, and phonon-assisted energy transfer between Ions in solids.Phys. Rev. B,1970, 1(7):2961-2969
[23]Heo J, Shin Y B. Absorption and mid-infrared emission spectroscopy of Dy3+ in Ge-As(or Ga)-S glasses.J. Non-Cryst. Solids,1996, 196(1/2/3):162-167

文章导航

/