基于石墨烯可饱和吸收体的掺铒光纤环形腔脉冲激光器

冯德军; 黄文育; 纪鹏宇; 姜守振; 隋青美

doi:10.3788/OPE.20132105.1097

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基于石墨烯可饱和吸收体的掺铒光纤环形腔脉冲激光器

现代应用光学 | 更新时间：2020-08-12

- 基于石墨烯可饱和吸收体的掺铒光纤环形腔脉冲激光器
- Erbium-doped fiber ring cavity pulsed laser based on graphene saturable absorber
- 光学精密工程 2013年21卷第5期页码：1097-1101
- 作者机构：
  
  山东大学信息科学与工程学院2. 山东师范大学物理与电子科学学院3. 山东大学控制科学与工程学院
- 作者简介：
- 基金信息：
  
  层数可控反射式石墨烯饱和吸收镜的制备及性能研究();双波长可切换的窄线宽线偏振掺Yb双包层光纤激光器的关键技术研究()
- DOI：10.3788/OPE.20132105.1097
  中图分类号： TN248.1
- 收稿日期：2012-10-24，
  
  修回日期：2013-01-22，
  
  网络出版日期：2013-05-24，
  
  纸质出版日期：2013-05-15
- 稿件说明：
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冯德军黄文育纪鹏宇姜守振隋青美. 基于石墨烯可饱和吸收体的掺铒光纤环形腔脉冲激光器[J]. 光学精密工程, 2013,21(5): 1097-1101

FENG De-jun HUANG Wen-yu JI Peng-yu JIANG Shou-zhen SUI Qing-mei. Erbium-doped fiber ring cavity pulsed laser based on graphene saturable absorber[J]. Editorial Office of Optics and Precision Engineering, 2013,21(5): 1097-1101
冯德军黄文育纪鹏宇姜守振隋青美. 基于石墨烯可饱和吸收体的掺铒光纤环形腔脉冲激光器[J]. 光学精密工程, 2013,21(5): 1097-1101 DOI： 10.3788/OPE.20132105.1097.

FENG De-jun HUANG Wen-yu JI Peng-yu JIANG Shou-zhen SUI Qing-mei. Erbium-doped fiber ring cavity pulsed laser based on graphene saturable absorber[J]. Editorial Office of Optics and Precision Engineering, 2013,21(5): 1097-1101 DOI： 10.3788/OPE.20132105.1097.

摘要

利用新型材料石墨烯作为可饱和吸收体，设计了用于光纤通信和材料加工的环形腔结构脉冲光纤激光器，实验研究了石墨烯可饱和吸收产生脉冲输出的原理以及输出脉冲激光的特性。通过激光诱导沉积法将石墨烯材料转移到光纤端面并将其置于环形激光腔结构中；采用974 nm半导体激光器作为抽运源，掺铒光纤作为增益介质，调节偏振控制器的角度得到了稳定的锁模输出脉冲。获得的锁模脉冲中心波长为1 560.1 nm，重复频率为7.89 MHz，脉冲光谱3 dB带宽为0.27 nm，脉冲宽度为14.7 ps。实验显示，由于石墨烯具有良好的可饱和吸收性能，损伤阈值比较高，有望取代单壁碳纳米管成为一种新型的激光锁模材料。

Abstract

A ring cavity fiber laser was proposed by using graphene as a saturable absorber for fiber optic communication and material processing. The principle how the grapheme could generate pulse trains and the laser output characteristics were studied experimentally. Then the laser induced deposition method was used to transfer the graphene to the fiber end face and place it in the ring laser cavity. By taking a 974 nm semiconductor laser as the pumping source and the Er3+-doped fiber as the gain medium

the laser generated stable pulse trains by changing the orientations of a polarizer above the threshold pump power. The experiment shows that the center wavelength of laser is 1 560.1 nm with a full width at half maximum spectrum of 0.27 nm and the pulse repetition rate is 7.89 MHz with a pulse width of 14.7 ps. It means that the graphene is expected to replace single-walled carbon nanotubes in pulsed laser applications as a novel mode-locked material because of its good saturable absorption properties and a higher damage threshold.

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references

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