Ge-Se基硫系玻璃在通信波段的三阶非线性与光谱特性研究

乔北京; 陈飞飞; 黄益聪; 戴世勋; 聂秋华; 徐铁峰

doi:10.7498/aps.64.154216

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摘要

在Ge-Se二元体系中引入相同摩尔比的Ga, Sn, Sb, Te四种元素, 使用熔融淬冷法制备了一系列硫系玻璃. 利用吸收光谱获得了不同元素引入下硫系玻璃能带结构的变化, 并结合拉曼光谱详细研究了产生光学特性变化的微观表征. 使用Z扫描方法测试了各个硫系玻璃样品在1550 nm波长下的三阶非线性参数, 发现加入Sn的玻璃的三阶非线性折射率n2最大, 达到了6.36×10-17 m2/W, 且其品质因子大于23, 表明Sn引入能够增强硫系玻璃在通信波段的三阶非线性, 这一研究结果为以后的高性能红外器件的设计及制备提供了一种环保且性能优良的候选材料.

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作者及机构信息

1.
宁波大学高等技术研究院红外材料及器件实验室, 宁波 315211

基金项目: 国家自然科学基金(批准号: 61435009, 61308094) 国家重点基础研究发展计划(973计划项目子课题)(批准号: 2012CB722703)和宁波大学王宽诚幸福基金.

参考文献

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[2]	Ren J, Li B, Wagner T, Zeng H, Chen G 2014 Opt. Mater. 36 911
[3]	Chen F F, Dai S X, Lin C G, Yu Q S, Zhang Q 2013 Opt Express 21 24847
[4]	Chen F, Yu Q, Qiao B, Xu T, Dai S, Ji W 2015 J. Non-Cryst. Solids. 412 30
[5]	Wang T, Gai X, Wei W, Wang R, Yang Z, Shen X, Madden S, Luther-Davies B 2014 Opt Mater Express 4 1011
[6]	Yang P L, Dai S X, Yi C S, Zhang P Q, Wang X S, Wu Y H, Xu Y S, Lin C G 2014 Acta Phys. Sin. 63 014210 (in Chinese) [杨佩龙, 戴世勋, 易昌申, 张培晴, 王训四, 吴越豪, 许银生林常规 2014 物理学报 63 014210]
[7]	Yu Y, Gai X, Wang T, Ma P, Wang R, Yang Z, Choi D Y, Madden S, Luther-Davies B 2013 Opt. Mater Express 3 1075
[8]	Guo H, Chen H, Hou C, Lin A, Zhu Y, Lu S, Gu S, Lu M, Peng B 2011 Mater. Res. Bull. 46 765
[9]	Hou Y, Liu Q, Zhou H, Gao C, Qian S, Zhao X 2010 Solid State Commun. 150 875
[10]	Petit L, Carlie N, Chen H, Gaylord S, Massera J, Boudebs G, Hu J, Agarwal A, Kimerling L, Richardson K 2009 J. Solid State Chem. 182 2756
[11]	Dong G, Tao H, Chu S, Xiao X, Wang S, Zhao X, Gong Q 2008 J. Non-Cryst. Solids. 354 440
[12]	Fayek S A 2005 Infrared Phys. Techn. 46 193
[13]	Tauc J,Menth A 1972 Journal of Non-Crystalline Solids 8 569
[14]	Sheik-Bahae M, Said A A, Wei TH, Hagan D J, Van Stryland E W 1990 IEEE J. Quantum Electron 26 760
[15]	Yin M, Li H, Tang S, Ji W 2000 Appl. Phys. B 70 587
[16]	Baeck J H, Kim T H, Choi H J, Jeong K H, Cho M H 2011 J. Phys. Chem. C 115 13462
[17]	Holomb R, Mitsa V, Akalin E, Akyuz S,Sichka M 2013 J. Non-Cryst. Solids. 373 51
[18]	Jackson K, Briley A, Grossman S, Porezag D V, Pederson M R 1999 Phys. Rev. B: Condens. 60 R14985
[19]	Han X, Tao H, Pan R, Lang Y, Shang C, Xing X, Tu Q, Zhao X 2013 Physics Procedia 48 59
[20]	Adam A B 2009 Journal of King Saud University-Science. 21 93

施引文献

[1]	Romanova E A, Kuzyutkina Y S, Konyukhov A I, Abdel-Moneim N, Seddon A B, Benson T M, Guizard S, Mouskeftaras A 2014 Opt. Eng 53 1
[2]	Ren J, Li B, Wagner T, Zeng H, Chen G 2014 Opt. Mater. 36 911
[3]	Chen F F, Dai S X, Lin C G, Yu Q S, Zhang Q 2013 Opt Express 21 24847
[4]	Chen F, Yu Q, Qiao B, Xu T, Dai S, Ji W 2015 J. Non-Cryst. Solids. 412 30
[5]	Wang T, Gai X, Wei W, Wang R, Yang Z, Shen X, Madden S, Luther-Davies B 2014 Opt Mater Express 4 1011
[6]	Yang P L, Dai S X, Yi C S, Zhang P Q, Wang X S, Wu Y H, Xu Y S, Lin C G 2014 Acta Phys. Sin. 63 014210 (in Chinese) [杨佩龙, 戴世勋, 易昌申, 张培晴, 王训四, 吴越豪, 许银生林常规 2014 物理学报 63 014210]
[7]	Yu Y, Gai X, Wang T, Ma P, Wang R, Yang Z, Choi D Y, Madden S, Luther-Davies B 2013 Opt. Mater Express 3 1075
[8]	Guo H, Chen H, Hou C, Lin A, Zhu Y, Lu S, Gu S, Lu M, Peng B 2011 Mater. Res. Bull. 46 765
[9]	Hou Y, Liu Q, Zhou H, Gao C, Qian S, Zhao X 2010 Solid State Commun. 150 875
[10]	Petit L, Carlie N, Chen H, Gaylord S, Massera J, Boudebs G, Hu J, Agarwal A, Kimerling L, Richardson K 2009 J. Solid State Chem. 182 2756
[11]	Dong G, Tao H, Chu S, Xiao X, Wang S, Zhao X, Gong Q 2008 J. Non-Cryst. Solids. 354 440
[12]	Fayek S A 2005 Infrared Phys. Techn. 46 193
[13]	Tauc J,Menth A 1972 Journal of Non-Crystalline Solids 8 569
[14]	Sheik-Bahae M, Said A A, Wei TH, Hagan D J, Van Stryland E W 1990 IEEE J. Quantum Electron 26 760
[15]	Yin M, Li H, Tang S, Ji W 2000 Appl. Phys. B 70 587
[16]	Baeck J H, Kim T H, Choi H J, Jeong K H, Cho M H 2011 J. Phys. Chem. C 115 13462
[17]	Holomb R, Mitsa V, Akalin E, Akyuz S,Sichka M 2013 J. Non-Cryst. Solids. 373 51
[18]	Jackson K, Briley A, Grossman S, Porezag D V, Pederson M R 1999 Phys. Rev. B: Condens. 60 R14985
[19]	Han X, Tao H, Pan R, Lang Y, Shang C, Xing X, Tu Q, Zhao X 2013 Physics Procedia 48 59
[20]	Adam A B 2009 Journal of King Saud University-Science. 21 93

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Ge-Se基硫系玻璃在通信波段的三阶非线性与光谱特性研究

1. 宁波大学高等技术研究院红外材料及器件实验室, 宁波 315211

基金项目:

国家自然科学基金(批准号: 61435009, 61308094) 国家重点基础研究发展计划(973计划项目子课题)(批准号: 2012CB722703)和宁波大学王宽诚幸福基金.

收稿日期: 2015-01-23

修回日期: 2015-04-20

刊出日期: 2015-08-05

摘要: 在Ge-Se二元体系中引入相同摩尔比的Ga, Sn, Sb, Te四种元素, 使用熔融淬冷法制备了一系列硫系玻璃. 利用吸收光谱获得了不同元素引入下硫系玻璃能带结构的变化, 并结合拉曼光谱详细研究了产生光学特性变化的微观表征. 使用Z扫描方法测试了各个硫系玻璃样品在1550 nm波长下的三阶非线性参数, 发现加入Sn的玻璃的三阶非线性折射率n2最大, 达到了6.36×10-17 m2/W, 且其品质因子大于23, 表明Sn引入能够增强硫系玻璃在通信波段的三阶非线性, 这一研究结果为以后的高性能红外器件的设计及制备提供了一种环保且性能优良的候选材料.

关键词:

Third-order optical nonlinearity at communication wavelength and spectral characteristics of Ge-Se based chalcogenide glasses

1.
Laboratory of Infrared Materials and Devices, The Research Institute of Advanced Technologies, Ningbo University, Ningbo 315211, China

Fund Project:

Project partially supported bythe National Natural Science Foundation of China (Grant Nos. 61435009, 61308094) National Program on Key Basic Research Project (973 Program) (Grant No. 2012CB722703), and K. C. Wong Magna Fund in Ningbo University.

Received Date: 23 January 2015

Accepted Date: 20 April 2015

Published Online: 05 August 2015

Abstract: A series of Ge-Se chalcogenide glasses incorporated with same molar percentage of Ga, Sn, Sb and Te are synthesized by melt-quenching method. The variations of optical band gaps doped with different elements are investigated by absorption spectra, and the relationship of optical band gap with glass network structure is studied by Raman spectra The results show that the doping of heavy metallic elements (except Ga) could reduce the optical band gap of the Ge-Se glass due to the decrease of the number of Se-Se chains or ring bonds. Third-order optical nonlinearities of the glasses are studied by femtosecond Z-scan method at a telecom wavelength of 1550nm. The results show that the performance of third-order optical nonlinearity of the Ge-Se glass could be improved by doping the above-mentioned elements. By comparison, the Sn-doped Ge-Se glass has a maximum nonlinear refraction index (n2) of 6.36× 10-17 m2/W and a figure of merit of over 23. By combining the experimental results from Raman spectra, the enhancement of third-order optical nonlinearity after the introduction of Sn can be ascribed to the formation of Sn(Se1/2)4 tetrahedra that enters into the main frame of Ge-Se glass and results in a stable Ge-Sn-Se network. Te doping could also remarkably enhance the n2 value of the Ge-Se glass, however, it could cause large two-photon absorption, leading to a poor value of figure of merit. The research result shows that chalcogenide glass in Ge-Sn-Se ternary system is an ideal candidate material for designing and fabricating infrared devices with high performance and environmental friendness.

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