Development of germanium gallium sulphide glass fibres for the 1.31 μm praseodymium-doped fibre amplifier

被引:30
作者
Schimmel, RC
Faber, AJ
de Waardt, H
Beerkens, RGC
Khoe, GD
机构
[1] Eindhoven Univ Technol, Telecommun Technol & Electromagnet Div, NL-5600 MB Eindhoven, Netherlands
[2] TNO, Inst Appl Phys, NL-5600 AN Eindhoven, Netherlands
[3] Eindhoven Univ Technol, Dept Chem Proc Engn, NL-5600 MB Eindhoven, Netherlands
关键词
D O I
10.1016/S0022-3093(01)00400-8
中图分类号
TQ174 [陶瓷工业]; TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
We report on our current progress in the development of germanium gallium sulphide glass fibres for the praseodymium-doped fibre amplifier (PDFA). Praseodymium-doped glasses with compositions (GeS8)(98)(GaS3)(2) (x: 2.25, 2.5, 3) are melted from germanium and gallium metals and sulphur in sealed silica ampoules at 1000 degreesC and then quenched in air. The critical step in the fibre manufacturing process is the fabrication of the fibre preform out of glass rods. The 'rod in tube' method was selected for preform fabrication. A new hot deformation process for manufacturing cladding tubes using the visco-elastic properties of the glass is described. A measure for the thermal stability of the glasses is the difference between the glass transition temperature, T-g, and the crystallisation onset temperature, T-g. The thermal stability was evaluated using dilatometry and combined differential thermal analysis/thermogravimetry (DTA/TG) analysis for determining T-g and T-g. For the selected germanium gallium sulphide glasses the difference between the crystallisation temperature and glass transition temperature is more than 200 degreesC. Both the fibre drawing temperature and the hot deformation temperature (to produce cladding glass tubes) are less than the crystallisation onset temperature. The germanium gallium sulphide host glasses are transparent in the 0.5-10 mum wavelength region. The wavelength of the maximum of the stimulated emission band with full width at half maximum (FWHM) amplitude of 80 nm is 1.34 mum, the emission lifetime is 390 mus. (C) 2001 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:188 / 192
页数:5
相关论文
共 9 条
[1]  
KALE BB, P 18 INT C GLASS
[2]  
KOBELKE J, 1998, C INFR GLASS OPT FIB, V3416
[3]   PR3+-DOPED FLUORIDE FIBER AMPLIFIER OPERATING AT 1.31 MU-M [J].
OHISHI, Y ;
KANAMORI, T ;
KITAGAWA, T ;
TAKAHASHI, S ;
SNITZER, E ;
SIGEL, GH .
OPTICS LETTERS, 1991, 16 (22) :1747-1749
[4]  
SCHOLZE H, 1988, GLAS STRUKTUR EIGENS
[5]   PR3+-DOPED GESX-BASED GLASSES FOR FIBER AMPLIFIERS AT 1.3-MU-M [J].
SIMONS, DR ;
FABER, AJ ;
DEWAAL, H .
OPTICS LETTERS, 1995, 20 (05) :468-470
[6]  
SIMONS DR, 1995, THESIS TU EINDHOVEN
[7]   Glass viscosity and structural relaxation by parallel plate rheometry using a thermo-mechanical analyser [J].
Wang, J .
MATERIALS LETTERS, 1997, 31 (1-2) :99-103
[8]   PR3+-DOPED GE-GA-S GLASSES FOR 1.3-MU-M OPTICAL-FIBER AMPLIFIERS [J].
WEI, K ;
MACHEWIRTH, DP ;
WENZEL, J ;
SNITZER, E ;
SIGEL, GH .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 1995, 182 (03) :257-261
[9]   A REVIEW OF RECENT SYSTEM DEMONSTRATIONS INCORPORATING 1.3-MU-M PRASEODYMIUM-DOPED FLUORIDE FIBER AMPLIFIERS [J].
WHITLEY, TJ .
JOURNAL OF LIGHTWAVE TECHNOLOGY, 1995, 13 (05) :744-760