Optical and Photoluminescence Properties of Erbium-Doped Chalcogenide Glasses (GeGaS:Er)

被引:27
作者
Kasap, Safa [1 ]
Koughia, Kirill [1 ]
Soundararajan, Gokulakrishnan [1 ]
Brik, Mikhail G. [2 ]
机构
[1] Univ Saskatchewan, Dept Elect & Comp Engn, Saskatoon, SK S7N 5A9, Canada
[2] Univ Tartu, Inst Phys, EE-51014 Tartu, Estonia
基金
加拿大自然科学与工程研究理事会;
关键词
Absorption and emission cross-section; chalcogenide glasses; radiative lifetime; rare-earth doping;
D O I
10.1109/JSTQE.2008.921415
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
We have examined the optical and photoluminescence (PL) properties of Er3+-doped GeGaS glasses of near-stoichiometric composition Ge28Ga6.2S65.3:Er-0.5. We have also used powdered samples of various mean sizes < L > to examine the dependence of the 1.54-mu m PL emission spectrum and the PL decay time on the average sample size. Optical absorption spectra of Er3+ ions arising from transitions between different energy manifolds, such as I-4(15/2)-I-4(13/2), I-4(15/2)-I-4(11/2), etc., have been used to extract Omega(2), Omega(4), and Omega(6) values using the Judd-Ofelt analysis and a Judd-Ofelt radiative lifetime T-JO = 2.6 ms for the I-4(13/2)-I-4(15/2) transition. The PL emission spectra and the decay time have been found to depend on the mean sample size. The spectra are broader and the decay times are longer for larger sample sizes, due to photon trapping occurring in the sample. The extrapolated decay time to zero particle size yields a decay time that matches the Judd-Ofelt radiative lifetime almost perfectly, and confirms the argument that the true PL lifetime needs to be measured in fine powders to avoid reabsorption effects. We have estimated the maximum emission cross section as 15.5 x 10(-21) cm(2).
引用
收藏
页码:1353 / 1360
页数:8
相关论文
共 70 条
[1]  
Aggarwal ID, 2002, J OPTOELECTRON ADV M, V4, P665
[2]  
[Anonymous], PHOTOINDUCED METASTA
[3]  
[Anonymous], 2003, AMORPHOUS SEMICONDUC
[4]   The interplay of self-trapping and self-quenching for resonant transitions in solids; role of a cavity [J].
Auzel, F ;
Bonfigli, F ;
Gagliari, S ;
Baldacchini, G .
JOURNAL OF LUMINESCENCE, 2001, 94 :293-297
[5]   Inhomogeneous and homogeneous linewidths in Er3+-doped chalcogenide glasses [J].
Bigot, L ;
Jurdyc, AM ;
Jacquier, B ;
Adam, JL .
OPTICAL MATERIALS, 2003, 24 (1-2) :97-102
[6]   Recent advances in chalcogenide glasses [J].
Bureau, B ;
Zhang, XH ;
Smektala, F ;
Adam, JL ;
Troles, J ;
Ma, HL ;
Boussard-Plèdel, C ;
Lucas, J ;
Lucas, P ;
Le Coq, D ;
Riley, MR ;
Simmons, JH .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 2004, 345 :276-283
[7]   Emission properties of the Er3+:4I11/2 → 4I13/2 transition in Er3+- and Er3+/Tm3+-doped Ge-Ga-As-S glasses [J].
Choi, YG ;
Kim, KH ;
Lee, BJ ;
Shin, YB ;
Kim, YS ;
Heo, J .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 2000, 278 (1-3) :137-144
[8]   High index contrast waveguides in chalcogenide glass and polymer [J].
DeCorby, RG ;
Ponnampalam, N ;
Pai, MM ;
Nguyen, HT ;
Dwivedi, PK ;
Clement, TJ ;
Haugen, CJ ;
McMullin, JN ;
Kasap, SO .
IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS, 2005, 11 (02) :539-546
[9]  
Desurvire E., 1994, ERBIUM DOPED FIBRE A
[10]   A THEORY OF SENSITIZED LUMINESCENCE IN SOLIDS [J].
DEXTER, DL .
JOURNAL OF CHEMICAL PHYSICS, 1953, 21 (05) :836-850