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2 μm Pulsed Fiber Laser Sources and Their Application in Terahertz Generation

机译:2μm脉冲光纤激光源及其在太赫兹产生中的应用

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摘要

In this dissertation, an all-fiber-based single frequency nanosecond pulsed laser system at ~ 1918.4 nm in master-oscillator-power-amplifier (MOPA) configuration is present. The nanosecond pulse seed is achieved by directly modulating a continuous wave (CW) single frequency fiber laser using a fast electro-optical modulator (EOM) driven by an arbitrary waveform generator (AWG). One piece of single mode, large core, polarization-maintaining (PM) highly thulium-doped (Tm-doped) germanate glass fiber (LC-TGF) is used to boost the pulse power and pulse energy of these modulated pulses in the final power amplifier. This laser system can work in both high power and high energy regime: in high power regime, to the best of our knowledge, the highest average power 16 W and peak power 78.1 kW are achieved for single frequency transform-limited ~2.0 ns pulses at 500 kHz and 100 kHz repetition rate, respectively: In high energy regime, nearly 1 mJ and half mJ pulse energy is obtained for ~15 ns pulses at 1 kHz repetition rate and 5 kHz repetition rate, respectively. Theoretical modeling of the large-core highly Tm-doped germanate glass double-cladding fiber amplifier (LC-TG-DC-FA) is also present for 2&mum nanosecond pulse amplification. A good agreement between the theoretical and experimental results is achieved. The model can simulate the evolution of pump power, signal energy, pulse shape and the amplified stimulated emission (ASE) in the amplifier. It can also be utilized to investigate the dependence of the stored energy in the LC-TGF on the pump power, seed energy and repetition rate, which can be used to design and optimize the LC-TG-DC-FA to achieve higher pulse energy and average power. Two channel of high energy nanosecond pulses (at 1918.4 nm and 1938 nm) are utilized to generate THz wave in a quasi-phase-matched (QPM) gallium arsenide (GaAs) based on difference frequency generation. THz wave with ~ 5.4μW average power and ~18 mW peak power has been achieved. Besides, one model is built to simulate a singly resonated THz parametric oscillator. The threshold, the dependence of output THz energy on pump energy has been investigated through this model. One pump enhanced THz parametric oscillator has been proposed. The enhancement factor of the nanosecond pulses in a bow-tie ring cavity has been calculated for different pulse duration, cavity length and the transmission of the coupler. And the laser resonances in the ring cavity have been observed by using a piezo to periodically adjust the cavity length. We also build an all-fiber thulium-doped wavelength tunable mode-locked laser operating near 2&mum. Reliable self-starting mode locking over a large tuning range (>50 nm) using fiber taper based carbon nanotube (FTCNT) saturable absorber (SA) is observed. Spectral tuning is achieved by stretching another fiber taper. To the best of our knowledge, this is the first demonstration of an all-fiber wavelength tunable mode-locked laser near 2&mum.
机译:本文提出了一种全光纤单频纳秒脉冲激光系统,其主振荡器功率放大器(MOPA)配置约为1918.4 nm。纳秒脉冲种子是通过使用由任意波形发生器(AWG)驱动的快速电光调制器(EOM)直接调制连续波(CW)单频光纤激光器获得的。一根高掺,(Tm掺杂)的德国锗玻璃纤维(LC-TGF)的单模,大芯,保偏(PM)用来提高最终功率中这些调制脉冲的脉冲功率和脉冲能量放大器。此激光系统可以在高功率和高能量状态下工作:据我们所知,在高功率状态下,单频变换限制〜2.0 ns的脉冲可实现最高平均功率16 W和峰值功率78.1 kW。分别为500 kHz和100 kHz重复频率:在高能量状态下,以15 kHz重复频率和1 kHz重复频率分别对〜15 ns的脉冲分别获得近1 mJ和一半mJ的脉冲能量。还存在用于2μm纳秒脉冲放大的大芯高Tm掺杂德国锗玻璃双包层光纤放大器(LC-TG-DC-FA)的理论模型。理论和实验结果之间取得了良好的一致性。该模型可以模拟放大器中泵浦功率,信号能量,脉冲形状和放大的受激发射(ASE)的演化。它也可用于研究LC-TGF中存储的能量对泵浦功率,种子能量和重复频率的依赖性,可用于设计和优化LC-TG-DC-FA以获得更高的脉冲能量和平均功率。利用两个通道的高能量纳秒脉冲(在1918.4 nm和1938 nm处),基于差​​频生成,在准相位匹配(QPM)砷化镓(GaAs)中生成THz波。已获得具有约5.4μW平均功率和约18mW峰值功率的太赫兹波。此外,建立了一个模型来模拟单谐振THz参数振荡器。通过该模型研究了阈值,输出太赫兹能量对泵浦能量的依赖性。已经提出了一种泵浦增强的THz参数振荡器。对于不同的脉冲持续时间,腔长和耦合器的传输,已经计算出领结环腔中纳秒脉冲的增强因子。并且已经通过使用压电来周期性地调节腔体长度来观察到环形腔体中的激光共振。我们还制造了在2μm附近工作的全光纤掺-波长可调锁模激光器。使用基于纤维锥形的碳纳米管(FTCNT)的可饱和吸收剂(SA),可以在较大的调谐范围(> 50 nm)上可靠地锁定自启动模式。通过拉伸另一种光纤锥度可以实现光谱调谐。据我们所知,这是2微米附近全光纤波长可调锁模激光器的首次演示。

著录项

  • 作者

    Fang Qiang;

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  • 年度 2012
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  • 原文格式 PDF
  • 正文语种 en
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