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Hybrid Nd~(3+)-doped passively Q-switched waveguide laser made by ion exchange

机译:杂交Nd〜(3 +) - 掺杂通过离子交换制成的被动Q开关的波导激光器

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In the mid 80's, the doping of optical fiber's core with rare earth atoms has been a major breakthrough in the field of optical telecommunications since it allowed the realization of in-line optical amplifiers. However, erbium-doped fiber amplifiers are a few meters long and a huge effort has been made in order to realize compact and efficient active devices based on rare-earth-doped waveguides. For this purpose the use of phosphate glasses instead of silicate ones has been investigated because they allow a better solubility of the inserted rare earths. In this paper we present the realization of a hybrid Neodymium-doped passively Q-switched waveguide laser made by ion exchange on a Schott IOG-1 phosphate laser glass combined with the deposition of a BDN saturable absorber diluted in a cellulose acetate polymer cladding. In a first step, we present the CW operation of the laser with an undoped cladding. We show that for a 3.5-μm wide, 1.4-cm long waveguide realized by a silver-sodium ion exchange, a 6 mW output has been achieved by creating a Fabry-Perot cavity with dielectric multilayers mirrors sticked to the chip facets. Then, the characterizations performed on the BDN doped layers are presented. It is shown that a proper selection of the hybrid guiding structure and saturable absorber concentration entail an excess absorption ranging from 1 to 10 dB/cm at zero flux. Finally, results on Q-switched behavior are presented. Optical pulse duration of 2-ns (FWHM) was obtained with repetition rates ranging from 5 to around 50 kHz for a 22 W pulse peak power.
机译:在80年代中期,具有稀土原子的光纤芯的掺杂是光电信领域的重大突破,因为它允许在线光放大器的实现。然而,掺铒光纤放大器长时间长,并且已经进行了巨大的努力,以实现基于稀土掺杂波导的紧凑型有效的有效器件。为此目的,已经研究了磷酸盐玻璃代替硅酸盐,因为它们允许插入的稀土溶解度更好。在本文中,我们介绍了通过离子交换的混合钕掺杂被动Q开关的波导激光器,与在纤维素醋酸纤维素聚合物包层中稀释的BDN可饱和吸收器的沉积结合。在第一步中,我们介绍了激光的CW操作,未掺杂的包层。我们表明,对于3.5微米的宽,由银钠离子交换实现的1.4厘米长的波导,通过产生带有粘附到芯片刻面的介电多层镜子的法布里 - 珀罗腔来实现6MW输出。然后,呈现在BDN掺杂层上执行的特征。结果表明,合适的混合引导结构和可饱和吸收浓度的选择需要在零通量下的1至10dB / cm的过量吸收。最后,提出了Q切换行为的结果。获得2-NS(FWHM)的光学脉冲持续时间,重复速率范围为5至约50kHz,对于22W脉冲峰值功率。

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