Laser-Induced Phase Transformation in Chalcogenide Glasses Investigated by Micro-Raman Spectrometer

武汉理工大学学报-材料科学版(英文版), 2014, 29(1): 9-12. doi: 10.1007/s11595-014-0858-y

^1, , ^2, , ^3, , ^4, , ^5, , ^6,

1.Laboratory of Infrared Materials and Devices , Advanced Technology Research Institute , Ningbo Univeristy , Ningbo 315211 , China

2.Laboratory of Infrared Materials and Devices , Advanced Technology Research Institute , Ningbo Univeristy , Ningbo 315211 , China

3.State Key Laboratory of Silicate Materials for Architecture(Wuhan University of Technology), Wuhan 430070, China

4.State Key Laboratory of Silicate Materials for Architecture(Wuhan University of Technology), Wuhan 430070, China

5.Laboratory of Infrared Materials and Devices , Advanced Technology Research Institute , Ningbo Univeristy , Ningbo 315211 , China

6.Laboratory of Infrared Materials and Devices , Advanced Technology Research Institute , Ningbo Univeristy , Ningbo 315211 , China

基金项目: State Key Laboratory of Silicate Materials for Architectures (Wuhan University of Technology)(SYSJJ2013-03) Funded in part by the the International Science & Technology Cooperation Program of China(2011DFA12040)

Laser-Induced Phase Transformation in Chalcogenide Glasses Investigated by Micro-Raman Spectrometer

LIN Changgui ^1, , LI Zhuobin ^2, , GU Shaoxuan ^3, , TAO Haizheng ^4, , DAI Shixun ^5, , NIE Qiuhua ^6,

1.Laboratory of Infrared Materials and Devices , Advanced Technology Research Institute , Ningbo Univeristy , Ningbo 315211 , China

2.Laboratory of Infrared Materials and Devices , Advanced Technology Research Institute , Ningbo Univeristy , Ningbo 315211 , China

3.State Key Laboratory of Silicate Materials for Architecture(Wuhan University of Technology), Wuhan 430070, China

4.State Key Laboratory of Silicate Materials for Architecture(Wuhan University of Technology), Wuhan 430070, China

5.Laboratory of Infrared Materials and Devices , Advanced Technology Research Institute , Ningbo Univeristy , Ningbo 315211 , China

6.Laboratory of Infrared Materials and Devices , Advanced Technology Research Institute , Ningbo Univeristy , Ningbo 315211 , China

Keywords： chalcogenide glass

参考文献

[1]	Changgui Lin;Laurent Calvez;Bruno Bureau .Second-order optical nonlinearity and ionic conductivity of nanocrystalline GeS2-Ga2S3-LiI glass-ceramics with improved thermo-mechanical properties[J].Physical chemistry chemical physics: PCCP,2010(15):3780-3787.
[2]	Petit L.;Carlie N.;Anderson T.;Jiyeon Choi;Richardson M.;Richardson K.C. .Progress on the Photoresponse of Chalcogenide Glasses and Films to Near-Infrared Femtosecond Laser Irradiation: A Review[J].IEEE journal of selected topics in quantum electronics: A publication of the IEEE Lasers and Electro-optics Society,2008(5):1323-1334.
[3]	I. Blonskyi;V. Kadan;O. Shpotyuk;M. Iovu;P. Korenyuk;I. Dmitruk .Filament-induced self-written waveguides in glassy As_4Ge_(30)S_(66)[J].Applied physics. B, Lasers and optics,2011(4):951-956.
[4]	M. Hughes;W. Yang;D. Hewak .Fabrication and characterization of femtosecond laser written waveguides in chalcogenide glass[J].Applied physics letters,2007(13):131113-1-131113-3-0.
[5]	Lin, CG;Tao, HZ;Wang, Z;Wang, B;Zang, HC;Zheng, XL;Zhao, XJ .Defect configurations in Ge-S chalcogenide glasses studied by Raman scattering and positron annihilation technique[J].Journal of Non-Crystalline Solids: A Journal Devoted to Oxide, Halide, Chalcogenide and Metallic Glasses, Amorphous Semiconductors, Non-Crystalline Films, Glass-Ceramics and Glassy Composites,2009(7):438-440.
[6]	Xiudi Xiao;Qiming Liu;Guoping Dong .Preparation and second harmonic generation of nanosized Sb2S3 doped silica glasses by the sol-gel process[J].Journal of Sol-Gel Science and Technology,2007(2):169-174.
[7]	Lin, C.;Calvez, L.;Tao, H.;Allix, M.;Morac, A.;Zhang, X.;Zhao, X. .Evidence of network demixing in GeS_2-Ga_2S_3 chalcogenide glasses: A phase transformation study[J].Journal of Solid State Chemistry,2011(3):584-588.

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