Figure-eight fibre lasers with NALM loops consisting of highly nonlinear dispersion shifted fibres for dense wavelength division multiplexing

D. Schmieder, P. Swart, A. Booysen
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引用次数: 5

Abstract

We describe 'Figure-of-Eight' fibre lasers with NALM (Nonlinear Amplifying Loop Mirror) loops of 100 m, 200 m 300 m highly nonlinear dispersion shifted fibre and 50 m photonic crystal fibre. Apart from the NALM loops the rest of the fibre lasers consisted of normal single-mode fibre (SMF28). The fibre lasers produced mode-locked and Q-switched pulses. By varying the length of the NALM loop we generated a variety of short and long stable high peak power and low peak power pulses in the range from 2 ns to 104 ns. The length of the pulses depends on the length of the NALM loop and the pump diode power. By changing the setting of the polarization controllers we can manipulate the amplitude of the pulses, produce high and low pulses, step pulses, double or multiple pulses. The period of the pulses is equal to the round trip time. We present pulse widths, pulse peak power and spectral measurements in dependence of the pump diode power, and discuss the shapes and spectra of the laser pulses with reference to the transmission curves.
图8光纤激光器与NALM环路组成的高度非线性色散位移光纤密集波分复用
我们描述了具有NALM(非线性放大环镜)环路的“八字”光纤激光器,该环路为100米、200米、300米高度非线性色散位移光纤和50米光子晶体光纤。除了NALM环路外,其余的光纤激光器由普通单模光纤(SMF28)组成。光纤激光器产生锁模和调q脉冲。通过改变NALM回路的长度,我们产生了各种短和长稳定的峰值功率和低峰值功率脉冲,范围从2ns到104ns。脉冲的长度取决于NALM回路的长度和泵浦二极管的功率。通过改变偏振控制器的设置,我们可以控制脉冲的振幅,产生高脉冲和低脉冲,阶跃脉冲,双脉冲或多脉冲。脉冲的周期等于往返时间。我们给出了脉冲宽度、脉冲峰值功率和光谱测量与泵浦二极管功率的关系,并参考透射曲线讨论了激光脉冲的形状和光谱。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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