高Yb3+/Er3+掺杂的磷基有源光纤材料的光谱性质

王玲玲; 于凤霞; 谭芳; 韩科选; 兰娇

doi:10.3788/fgxb20143501.0090

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高Yb³⁺/Er³⁺掺杂的磷基有源光纤材料的光谱性质

器件制备及器件物理 | 更新时间：2020-08-12

- 高Yb³⁺/Er³⁺掺杂的磷基有源光纤材料的光谱性质
- Spectral Properties of Yb³⁺/Er³⁺ High Doped Rate Phosphorus Based Active Fiber Material
- 发光学报 2014年35卷第1期页码：90-95
- 作者机构：
  
  1. 长春理工大学材料科学与工程学院, 吉林长春 130022
  2. 长春大学理学院, 吉林长春 130022
  3. 山西长城微光器材股份有限公司,山西太原,030032
- 作者简介：
- 基金信息：
  
  国家科技重大专项（GFZX02030202.4）();国家科技创新基金（10c26212200507）资助项目()
- DOI：10.3788/fgxb20143501.0090
  中图分类号： TQ171.35
- 收稿日期：2013-08-13，
  
  修回日期：2013-09-08，
  
  纸质出版日期：2014-01-03
- 稿件说明：
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王玲玲, 于凤霞, 谭芳, 韩科选, 兰娇. 高Yb3+/Er3+掺杂的磷基有源光纤材料的光谱性质[J]. 发光学报, 2014,35(1): 90-95

WANG Ling-ling, YU Feng-xia, TAN Fang, HAN Ke-xuan, LAN Jiao. Spectral Properties of Yb3+/Er3+ High Doped Rate Phosphorus Based Active Fiber Material[J]. Chinese Journal of Luminescence, 2014,35(1): 90-95
王玲玲, 于凤霞, 谭芳, 韩科选, 兰娇. 高Yb3+/Er3+掺杂的磷基有源光纤材料的光谱性质[J]. 发光学报, 2014,35(1): 90-95 DOI： 10.3788/fgxb20143501.0090.

WANG Ling-ling, YU Feng-xia, TAN Fang, HAN Ke-xuan, LAN Jiao. Spectral Properties of Yb3+/Er3+ High Doped Rate Phosphorus Based Active Fiber Material[J]. Chinese Journal of Luminescence, 2014,35(1): 90-95 DOI： 10.3788/fgxb20143501.0090.

摘要

研究了Yb

/Er

共掺60P

-15BaO-10Al

-5ZnO-10

O（

=Na，K）以P

为主体的磷基有源光纤材料的光谱性质，以及不同Yb

/Er

掺杂浓度对光谱性质的影响规律。当Er

浓度为9.10010

/cm

、Yb

的掺杂浓度为5.40710

/cm

、Yb

/Er

浓度比为6：1时，玻璃样品在1 531 nm处的受激发射截面最大，为6.1710

-21

。同时，其荧光寿命为9.73 ms，荧光半高宽为53.16 nm，发射截面与半高宽的乘积为3.2810

-32

，综合性能最佳。

Abstract

/Er

co-doped 60P

-15BaO-10Al

-5ZnO-10

=Na

K) phosphorus based material with P

as the principal ingredient were researched. The spectroscopic properties of the fiber material and the effect of Yb

/Er

concentration ratios on the spectral properties were researched. When Er

concentration is 9.10010

/cm

concentration is 5.40710

/cm

and their optimum concentration ratio is 6:1

the largest stimulated emission cross section is obtained for 6.1710

-21

. At the meantime

the fluorescence lifetime is 9.73 ms

full width half maximum (FWHM) is 53.16 nm

and the product of emission cross section and FWHM is 3.2810

-32

which indicates this material has the best performance.

关键词

Keywords

references

Qian Q, Yang Z M. Development of Yb3+ doped phosphate glass fiber and 1.06 m single frequency laser[J]. Acta Optica Sinica (光学学报), 2010, 30(7):1904-1909 (in Chinese).[2] Lou Q H, Zhou J, Zhu J Q, et al. Research progress of high power fiber laser[J]. Infrared and Laser Engineering (红外与激光工程), 2006, 35(2):135-13 (in Chinese).[3] Shen R S, Zhang S Y, Du G T. Research progress of fiber laser[J]. Semicond. Optoelect.(半导体光电), 2009, 30(1):1-5 (in Chinese).[4] Jiang C, Liu H, Zeng Q, et al. Yb phosphate laser glass with high emission cross-section[J]. Phys. Chem. Solids, 2000, 61(8):1217-1223.[5] Norderhaug L, Olafsen T, Michaelsen T E, et al. Transmission loss characteristics of fluoro phosphate optical fibersin the ultraviolet to visible wavelength region[J]. Non-Cryst. Solids, 1997, 215(1):11-20.[6] Dai S X, Hu L L, Liu Z P, et al. Spectrum and laser properties of ytterbium doped phosphate glass at low temperature[J]. Acta Optica Sinica (光学学报), 2002, 22(5):627-631 (in Chinese).[7] Zhang W, Zhu J Q. Experimental investigation onsurface/subsurface damage of Nd-doped phosphate glass[J]. Acta Optica Sinica (光学学报), 2008, 28(2):268-272 (in Chinese).[8] Hu Y, Jiang S. Performance of high-concentration Er3+/Yb3+-codoped phosphate glass fiber amplifiers[J]. IEEE Photon. Tech. Lett., 2001, 13(7):657-659.[9] Lafond C, Osouf J, Laperle P, et al. Er3+-Yb3+ co-doped phosphate glass optical fiber for application at 1.54 microns[J]. SPIE, 2006, 6343:63430M-1-9.[10] Yin H R, Zhang C X, Liu L Y. Applications of differential thermal analysis in glass[J]. Ceramic (陶瓷), 2008, 6(1):14-18 (in Chinese).[11] Wang J. Study on the material of rare earth droped germanium glass infrared optical fiber[D]. Changchun University of Science and Technology, 2008 (in Chinese).[12] Niu Y. Study on the preparation and properties of rare-earth doped bismuth fluoroborate glass[D]. Qingdao: Ocean University of China, 2008 (in Chinese).[13] McCumber D E. Theory of photon-terminated optical masers[J]. Phys. Rev. A, 1964, 134(2):299-306.[14] Li W N, Zou K S, Lu M, et al. Synthesis and spectral properties of Yb3+ doped silicate glass system[J]. Spectrosc. Spect. Anal.(光谱学与光谱分析), 2006, 26(6):983-986 (in Chinese).[15] Desirena H, De la Rosa E, Diaz-Torres L A, et al. Concentration effect of Er3+ ion on the spectroscopic properties of Er3+ and Yb3+/Er3+ co-doped phosphate glasses[J]. Opt. Mater., 2006, 28(5):560-568.[16] Weber M J, Lynch J E, Blackburn D H, et al. Dependence of the stimulated emission cross section of Yb3+ on host glass composition[J]. Quant. Elect., 1983, 19:1600-1608.[17] Zhang W, Zhu J Q. Experimental study on the surface/sub surface damage properties of Nd doped phosphate glass[J]. Acta Optica Sinica (光学学报), 2008, 28(2):268-272 (in Chinese).[18] Wen S S, Feng Z M, Liu E H, et al. Investigation on fluorescence lifetime in the Yb3+-doped phosphate glasses[J]. Chin. J. Quant. Elect.(量子电子学报), 2004, 21(4):419-424 (in Chinese).[19] Li M H, Hu H F, Qi C H. A method to calculate the emission cross section of rare-earth ions[J]. Acta Optica Sinica (光学学报), 2001, 21(5):626-629 (in Chinese).[20] Jiang X W, Qiu J R, Zhu C S, et al. ESR studies and thresholds of femtosecond laser induced darkening in glasses[J]. Acta Phys. Sinica (物理学报), 2001, 50(5):871-874 (in Chinese).[21] Guo Y B, Wang T S, Li J, et al. Super fluorescence studies of erbium ytterbium co-doped fiber[J]. Semiconductor Optoelect.(半导体光电), 2004, 25(1):39-42 (in Chinese).

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