首页> 外文会议>Laser resonators, microresonators, and beam control XVI >Investigation of the low power stage of an 1178 nm Raman system
【24h】

Investigation of the low power stage of an 1178 nm Raman system

机译:研究1178 nm拉曼系统的低功率级

获取原文
获取原文并翻译 | 示例

摘要

An 1178 nm seeded and 1069 nm pumped Raman laser system where the second Stokes is amplified in a 1121 nm resonator defined by high reflector fiber Bragg gratings (FBGs) has the potential of producing high output power of narrow linewidth 1178 nm. However, 1121 nm power leakage out of the resonator cavity around the gratings was found to impact the performance of the laser and needs to be dealt with in order to obtain high 1178 nm output power levels. In order to address this problem, the causes of linewidth broadening must be understood. A fully nonlinear model has been built which involves propagation of the spectral wave shape via the nonlinear Schrodinger equation in addition to the Raman processes. It was found that increases in 1121 nm cavity power, fiber Bragg grating bandwidth, and the nonlinear index of refraction n_2, as well as a decrease in group velocity dispersion β_2 leads to an increase in linewidth broadening. It is concluded that the magnitude of linewidth broadening seen experimentally can only be explained if the spectral components outside the bandwidth of the FBGs are being amplified. Experimentally, 1121 nm power leakage can be handled by using a three wavelength WDM on either side of the rare earth doped amplifier. In addition, usage of a fiber having a high value for group velocity dispersion and/or a low value for nonlinear index of refraction n_2 in addition to narrower bandwidth fiber Bragg gratings may help reduce the amount of linewidth broadening.
机译:1178 nm种子和1069 nm抽运的拉曼激光器系统,在由高反射光纤布拉格光栅(FBG)定义的1121 nm谐振器中放大了第二斯托克斯,有可能产生窄线宽1178 nm的高输出功率。然而,发现从光栅周围的谐振腔漏出1121 nm的功率会影响激光器的性能,因此需要处理以获得高1178 nm的输出功率。为了解决这个问题,必须理解线宽加宽的原因。已经建立了一个完全非线性的模型,除了拉曼过程外,还包括通过非线性Schrodinger方程传播光谱波形的过程。发现1121nm腔功率,光纤布拉格光栅带宽和非线性折射率n_2的增加,以及群速度色散β_2的减小导致线宽加宽的增加。结论是,只有放大了FBG带宽之外的频谱分量后,才能解释实验观察到的线宽加宽幅度。实验上,可以通过在稀土掺杂放大器的任一侧使用三波长WDM来处理1121 nm的功率泄漏。此外,除了带宽较窄的光纤布拉格光栅之外,使用具有较高的群速度色散值和/或较低的非线性折射率n_2值的光纤可以帮助减少线宽加宽的量。

著录项

  • 来源
  • 会议地点 San Francisco CA(US)
  • 作者单位

    Air Force Research laboratory, Directed Energy Directorate, 3550 Aberdeen Avenue SE, Kirtland AFB,NM 87117,USA;

    Department of Computer and Electrical Engineering, MSC01 1100, 1 University of New Mexico,ECE Building, Room 125, Albuquerque, NM 87131-0001;

    College of Optical Sciences, University of Arizona, 1630 E. University Blvd, Tucson, AZ 85721;

    Air Force Research laboratory, Directed Energy Directorate, 3550 Aberdeen Avenue SE, Kirtland AFB,NM 87117,USA;

    Department of Computer and Electrical Engineering, MSC01 1100, 1 University of New Mexico,ECE Building, Room 125, Albuquerque, NM 87131-0001;

  • 会议组织
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Raman laser; resonator cavity; narrow linewidth; nonlinear Schroedinger equation;

    机译:拉曼激光谐振腔窄线宽非线性薛定inger方程;

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号