首页> 外文会议>IEEE LEOS Annual Meeting Conference >Tunable Er{sup}3+-doped fiber amplifiers covering S- and C + L-bands (1490 ~ 1610 nm) using discrete all-fiber ASE suppressing filters
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Tunable Er{sup}3+-doped fiber amplifiers covering S- and C + L-bands (1490 ~ 1610 nm) using discrete all-fiber ASE suppressing filters

机译:可调谐ER {SUP} 3 +拆卸的光纤放大器,使用离散全光纤ASE抑制滤波器覆盖S-和C + L波段(1490〜1610nm)

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S-band (1480 ~ 1520 nm) has been recently studied as a new frequency band for fiber-optic communication. So far, the most promising S-band EDFAs employ the EDFs with depressed inner cladding to achieve fundamental-mode cutoff λ{sub}c at the longer wavelengths [1]. The depressed inner cladding in EDFs modifies the waveguide dispersion, which in terms varies the refractive index dispersion (RID) n(λ) curves. The effective indices of the longer (shorter) wavelengths become lower (higher) than the index of the outer silica cladding respectively. The ASE at the longer wavelengths can then be substantially suppressed so that in the shorter wavelengths (S-band) higher population inversion and sufficient amplification can be obtained. The λ{sub}c can be tuned toward shorter wavelengths by bending the fiber and the total distributed loss for wavelengths longer than the λ{sub}c can be > 200 dB through an entire 15-m-long EDF. However, a specially designed EDF is required for S-band amplification and the cutoff efficiency and insertion loss become worse and higher, respectively, when the radius of bending curvature gradually decreases [1]. In contrast to the λ{sub}c induced by waveguide dispersion, we have demonstrated widely tunable (1250 ~1650 nm) side-polished fiber short-pass filters based on material dispersion [2]. The λ{sub}c is thermo-optically tunable (no moving part) and the high cutoff efficiency (deep stopband and sharp filter skirt) can still be maintained while tuning to different wavelengths. The short-pass filter can be further incorporated into the ring cavity of an EDF to locally suppress the unwanted wavelengths and achieve a high efficiency tunable fiber laser. However, a single local λ{sub}c is inefficient for the standard EDFs (no depressed inner cladding) to be operated as an amplifier at the shorter wavelengths (S-band) of the gain bandwidth. Consequently, we employ multistage tunable fused-tapered fiber short-pass filters discretely located in the standard silica-based EDF to achieve S-band amplification [3] in this work.
机译:最近已经研究了S-BAND(1480〜1520nm)作为光纤通信的新频段。到目前为止,最有前途的S频段EDFA采用EDFS凹陷内包层,以实现较长波长的基本模式截止λ{Sub} C [1]。 EDF中的凹陷内包层改变了波导分散体,其在术语中变化折射率分散(RiD)N(λ)曲线。较长(较短)波长的有效索引分别比外部二氧化硅包层的指数更低(更高)。然后可以基本上抑制较长波长的ASE,使得在较短的波长(S波长)中,可以获得更高的人口反转和足够的放大。通过弯曲光纤和比λ{sub} c长的波长的总分布式损耗可以通过整个15-m-long edf来调谐λ{sub} c。然而,当弯曲曲率半径逐渐降低时,S频带放大需要特殊设计的EDF,并且截止效率和插入损耗分别变得更差,并且分别更高。与波导分散诱导的λ{亚} C对比,我们已经展示了基于材料色散的广泛调谐(1250〜1650nm)侧抛光的纤维短通滤光片[2]。 λ{Sub} C是热光学调谐(无移动部件),并且在调谐到不同波长的同时仍然可以保持高截止效率(深止挡和锋利的滤网裙)。短通滤光器可以进一步结合到EDF的环形腔中,以局部抑制不需要的波长并实现高效率可调光纤激光器。然而,单个本地λ{Sub} C对于在增益带宽的较短波长(S波长)处作为放大器操作的标准EDF(无凹陷内部包层)效率低。因此,我们采用多级可调熔锥形纤维短通滤光片,位于标准二氧化硅的EDF中,以实现这项工作中的S波段放大[3]。

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