以亚本征腔往返间隔从啁啾锁模激光二极管发出的250 fs脉冲序列

N. Stelmakh, A. Azouz, J. Lourtioz
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引用次数: 0

摘要

据我们所知,在短脉冲锁模扩展腔激光二极管中,脉冲结构随外腔长度的精细周期性演变从未被报道过。在本文中,我们证明了当使用外部啁啾补偿时,这些锁模激光系统中的外部和本征腔长度之间存在很强的相互依赖性。我们发现外腔长度(l/sub e/)必须等于本征激光二极管腔长度(l/sub i/)的一个倍数,才能产生每本征腔往返时间有一个子脉冲的标准脉冲结构。同样,外腔长度必须等于(m+1/n)*l/sub i/,其中m为整数,才能获得每本质腔往返时间内的n个子脉冲。在我们的实验中,我们观察到n到8时明显的脉冲结构。后一个值对应于产生/spl sim/250 fs脉冲序列,脉冲重复率为/spl sim/300 GHz,总能量为/spl sim/20-30 pJ。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Trains of 250 fs pulses at sub-intrinsic-cavity roundtrip intervals from chirped mode-locked laser diodes
To our knowledge, fine periodical evolutions of the pulse structure with the length of the external cavity have never been reported in short-pulse mode-locked extended-cavity laser diodes. In this communication, we demonstrate a strong inter-dependence between the external and intrinsic cavity lengths in these mode-locked laser systems when an external chirp compensation is used. We found that the length of the external cavity (l/sub e/) must be equal to a multiple of the intrinsic laser diode cavity length (l/sub i/) to produce standard pulse structures with one sub-pulse per intrinsic cavity roundtrip time. Similarly, the external cavity length must be equal to (m+1/n)*l/sub i/, with m being an integer, to obtain n sub-pulses per intrinsic cavity roundtrip time. In our experiments, we observed pronounced pulse structures for n up to 8. This latter value corresponds to the generation of /spl sim/250 fs pulse trains with a pulse repetition rate of /spl sim/300 GHz and a total energy /spl sim/20-30 pJ.
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