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1.
李丽娜 《发光学报》2001,22(1):85-87
采用980nm无铝InGaAs/InGAsP/InGaP高功率量子阱激光器泵浦掺铒光纤放大器。在泵浦功率为20mW时,增益为33dB,最大增益系数6.7dB/mW,饱和输出功率为6dBm,并给出掺铒光纤长度和泵浦功率与增益特性的关系。以及输出功率与增益特性的关系。  相似文献   

2.
提出了一种基于环形芯铒离子部分掺杂光纤的涡旋光纤放大器。针对该掺铒光纤的放大特性,研究了光纤长度、掺铒浓度与抽运功率对信号模式增益特性的影响。研究结果表明,该光纤放大器能够支持22个轨道角动量模式稳定传输,且C波段(1530~1565 nm)所有信号模式增益大于23 dB,信噪比高于27 dB,差分模式增益小于0.015 dB。所提出的基于环形芯光纤的涡旋光纤放大器具有支持轨道角动量模式数量多、差分模式增益低、信噪比高的优势,对于OAM复用长距离传输系统中的在线放大具有重要参考价值。  相似文献   

3.
光纤光栅增益平坦化器件的研究   总被引:3,自引:1,他引:2  
采用幅度掩模和程控扫描曝光技术在经过氢载敏化处理的普通单模光纤上研制出了可用于实现掺铒光纤放大器增益谱平坦化的长周期光纤光栅器件。该器件使掺铒光纤放大器在30 nm带宽上的增益谱波动从±3 dB减小为±0.3 dB, 器件的附加损耗小于0.3 dB。  相似文献   

4.
In this paper, the variational method is employed for minimizing the gain ripple of multi-wavelength fiber Raman amplifiers. The variance of gain spectrum of the fiber Raman amplifier is regarded as the cost function, restriction on total pump power and average gain is given as the constraints of the minimization problem. It is shown that the minimization problem with any necessary constraints on the pump powers, average gain and signal to noise ratio, is reduced to a two-point boundary value problem. The method gives the entire possible local and global solutions. The method is applied to different examples of fiber Raman amplifiers with different lengths from 25 km to 100 km and different numbers of pumps from 4 to 20 to determine the pump powers and wavelengths for minimum gain ripple. It was obtained for a 100 km fiber Raman amplifier the gain ripple can be about 0.1 dB with on-off gain more than 20 dB.  相似文献   

5.
We investigate two configurations of Raman fiber amplifier in the 1530-1570 nm region. The gain spectrum variation is decreased from 8.31 dB to 2.48 dB when appropriately adjust the individual two pumps and optical fiber.  相似文献   

6.
Double-pass short-wavelength band erbium-doped fiber amplifier (S-band EDFA) with enhanced gain and noise figure characteristics is demonstrated. It uses a broadband fiber Bragg grating (FBG) operating in conventional-band (C-band) region to reduce the C-band amplified spontaneous emission (ASE) in the amplifier system and thus increases the population inversion in the S-band region. The small signal gain is increased by about 2.7 dB for 1500 nm signal at pump power of 103 mW, compared with that of the conventional double-pass amplifier without the FBG. The corresponding noise figure is also improved by 0.5 dB.  相似文献   

7.
Novel small Raman gain measurement method for installed fiber optic cables using a modulated pump light is proposed.We have demonstrated accurate Raman gain measurement in small Raman gain less than 1dB and we also measured Raman gain for the installed fiber optic cable by using average pumping power of about only 25mW.  相似文献   

8.
提出了结构简单的光纤布喇格光栅(FBG)双波长全光自动增益箝制方案,并进行了相关实验.结果表明,在三种不同的箝制波长组合1535.64nm+1562.68nm、1530.48nm+1562.68nm、1530.48 nm+1551.36 nm条件下,1540 nm信号的输出增益大小和输入信号功率动态范围几乎一致.对应此三种箝制波长组合,环路内的损耗分别为:14.7 dB、15 dB、15 dB.由此证明,在相同泵浦条件和环路损耗条件下,此三种不同箝制波长组合具有近似相同的箝制效果.而1551.36 nm+1562.68 nm箝制波长组合得到的结果相差甚远.此结果说明,在设计双波长全光自动增益箝制掺铒光纤放大器(OAGC-EDFA)时,为了取得足够大的信号增益,两箝制波长的波长间隔应尽量较大.  相似文献   

9.
WDM用增益平坦的高增益低噪声双段级联掺铒光纤放大器   总被引:6,自引:4,他引:2  
给出了设计波分复用(WDM)用高增益、低噪声和宽带宽增益平坦的双段级联掺铒光纤放大器(EDFA)的一般步骤和方法.通过优化设计各种参量,研制出了一台高增益、低噪声和宽带宽增益平坦的双段级联EDFA样机,实现了从1524.8~1561.4 nm共36.6 nm带宽内±0.325 dB的平坦增益,0 dBm输入时,饱和输出功率大于15 dBm的高功率输出;噪声指数低于5 dB.  相似文献   

10.
掺铒光纤放大器在光通信中有着广泛的应用。根据掺铒光纤的性能要求设计了合理的折射率剖面图,制备了高增益的掺铒光纤,在1530nm的吸收达到22dBm,在980nm泵浦光的吸收达到12dBm。其平坦增益带宽范围为1490—1560nm。  相似文献   

11.
双包层掺染料聚合物光纤放大器的增益性能分析   总被引:3,自引:2,他引:1  
李炳新  于荣金 《光子学报》2005,34(10):1466-1472
双包层聚合物光纤放大器可以减小染料的热漂白,使用速率方程的方法,给出了一个能够全面描述双包层掺染料聚合物光纤放大器增益性能的模型,模型既考虑了染料三重态能级对速率方程的影响,又考虑了双包层结构对泵浦光的影响,可以在稳态的情况下计算放大器的各种增益性能指标.  相似文献   

12.
In this article, we propose a novel superstructure fiber Bragg grating (SFBG)-based comb gain equalizer for fiber-optical parametric amplifiers (FOPAs). The target spectrum of the gain equalizer is obtained by two steps. Initially, we calculate the spectrum according to the inverse of the gain spectrum of the FOPA. Then we apply a channel-by-channel windowing method to shape each channel and adopt a Gaussian hypergeometric function to describe the rising and descending edges of each channel. The SFBG is finally synthesized with layer-peeling inverse scattering technique. Using the designed SFBG, the gain variation of the FOPA is flattened to be within ±0.4 dB for 16 ITU channels and the best channel isolation is as high as 35 dB. It should be pointed out that the proposed method could also be used to design gain equalizers for other optical amplifiers.  相似文献   

13.
一种基于新型长周期光纤光栅的动态增益均衡器   总被引:9,自引:5,他引:4  
报道了一种用高频CO2激光脉冲写出的长周期光纤光栅的温度特性和弯曲特性.实验表明,这种长周期光纤光栅的波长漂移随温度的变化呈线性关系,它的透射峰幅值变化随弯曲量的变化也呈线性关系.基于这两种线性关系,通过控制新型长周期光纤光栅的谐振峰位置和幅度,动态平坦了一组掺铒光纤放大器增益谱线.实验结果表明在C波段32nm范围内掺铒光纤放大器增益谱线平坦度可动态调整为±0.7dB.  相似文献   

14.
A gain and gain-flatness improved L-band dual-pass Raman fiber amplifier (RFA) utilizing a photonic crystal fiber (PCF) as gain medium is demonstrated. By introducing complementary gain spectra of typical forward and backward pumping single-pass RFA using the same PCF, we finally achieve average net gain level of 22.5 dB with a ±0.8 dB flattening gain in 20-nm bandwidth from 1595 nm to 1615 nm, which is rare in RFAs with only one single pump and no flattening filter. Compared with the single-pass pump configurations, gain level, flatness and bandwidth are greatly improved by using the dual-pass amplification configuration. The limitation of this configuration caused by multi-path interference (MPI) noise and stimulated Brillouin scattering (SBS) is also discussed.  相似文献   

15.
低噪声、高增益的L -band EDFA的实验研究   总被引:3,自引:3,他引:0  
秦山  强则煊  何赛灵 《光子学报》2005,34(3):409-411
针对传统的L-band EDFA的工作效率低,提出了一种基于单根光纤光栅、泵浦分配、两段级联的EDFA的新结构,其中的光纤光栅用来反射无用的后向C-band ASE.系统地研究了泵浦比例和光纤光栅波长对增益噪声指数的影响关系.最后经实验验证,得到了低噪声、高增益的L-band的EDFA.其在输入信号光(1570 nm)功率为-30 dBm及泵浦功率为70 mW时,增益为22.26 dB,增益噪声指数为4.96 dB.  相似文献   

16.
Using feedback theory, we analyze the gain of an all-optical gain-clamped praseodymium-doped fluoride fiber amplifier (AOGC PDFFA) for eight-channel multiwavelength operation. We demonstrate by numerical simulation that gain stabilization is achieved when the open-loop gain is higher than the feedback path attenuation. If this condition is fulfilled, the gain stabilizes to a value equal to the feedback path attenuation and is not influenced by the pump power, input signal power, number of channels, doped fiber length, or any other doped fiber parameter. In our setup the AOGC PDFFA noise figure is 0.12 dB lower than the open-loop PDFFA noise figure.  相似文献   

17.
We demonstrate a novel gain-flattening filter based on all fiber Mach-Zehnder interferometers for Sb-doped silica hybrid EDFA. A gain flatness of better than 0.9dB has been achieved for three concatenated filters in C-band.  相似文献   

18.
In this paper the gain characteristics of two-pump fiber optical parametric amplifiers (FOPA) with two-section highly nonlinear fibers are analyzed numerically and the parameters of the fibers are optimized to reach broad and flat gain spectra using genetic algorithm. Different from the previous methods, here the space between two pump wavelengths and the parameter β4 of the fibers are included as a pivotal factor in the optimization. The numerical simulation shows that using two-section practical high nonlinear fibers, the amplifier may reach 110 nm bandwidth covering 1495–1605 nm with 10.5 dB average gain and gain ripple of 0.17 dB, when the total pump power is 1 W.  相似文献   

19.
An erbium-doped fiber amplifier (EDFA) is simulated. The variation of gain with different parameters is obtained and the values of these parameters are optimized to achieve a maximum value of gain. A two-stage gain-flattened EDFA consisting of two EDFAs in series is also simulated. In the operating range of 1565-1610 nm, the flat gain of 46 dB is obtained.  相似文献   

20.
A highly efficient gain-clamped L-band EDFA with improved noise figure characteristic is demonstrated by simply adding a broadband C-band FBG in double-pass system. The combination of the FBG and optical circulator has created laser in the cavity for gain clamping. By adjusting the power combination of pumps 1 and 2, the clamped gain level can be controlled. The amplifier gain is clamped at 28.1 dB from −40 to −25 dBm with a gain variation of less than 0.5 dB by setting the pumps 1 and 2 at 59.5 and 50.6 mW, respectively. The gain is also flat from 1574 nm to 1604 nm with a gain variation of less than 3 dB. The corresponding noise figure varies from 5.6 to 7.6 dB, which is 0.8 to 2.6 dB less than those of unclamped amplifier.  相似文献   

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