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1.
掺铒光纤吸收增加光学双稳态   总被引:2,自引:1,他引:1  
张远程  宋骞 《光学学报》1998,18(10):459-1463
报道了的掺铒光纤中观测到的吸收增加非线性和无腔光学双稳运转。双稳是低功率的(亚毫瓦级)。分析了掺铒光纤吸收增加双稳态产生的机理  相似文献   

2.
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   

3.
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   

4.
种兰祥  李建郎 《光子学报》2007,36(9):1574-1577
研究了在掺镱光纤激光器中观察到的光学双稳态现象.激光信号光和驻留泵浦光的双稳特性来源于激光器在小信号和增益饱和两种情况下,掺镱光纤对信号的非线性吸收导致的激光器内腔非线性损耗.同时分析了把泵浦光中的光学双稳行为通过分叉的腔结构扩展到切换式双波长光纤激光器的可行性.  相似文献   

5.
掺铒光纤放大器的增益带宽是限制光纤通信系统传输容量提升的重要因素.受铒离子激发态吸收所限,常规L波段掺铒光纤难以实现更长波段的带宽扩展.本文基于改进的化学气相沉积工艺成功制备了P/Al共掺石英基L波段扩展掺铒光纤,研究了共掺离子对于铒离子4I13/2能级到4I9/2能级激发态吸收的影响.通过分别搭建单级前向泵浦和多级的放大结构,测试了其宽带放大性能.基于前向980 nm泵浦的单级结构,当输入信号功率为–9 dBm,泵浦功率为530 mW时,该光纤在1625.3 nm处增益达10.5 dB,最大噪声指数为5.9 dB.多级放大结构下,该光纤在1625.3 nm处增益可达23.4 dB.实验结果表明P/Al共掺石英基掺铒光纤可以有效抑制铒离子的激发态吸收,为进一步扩展L波段增益带宽提供了强有力的可行方案.  相似文献   

6.
15波长输出的布里渊掺铒光纤激光器   总被引:8,自引:3,他引:5  
多波长布里渊掺铒光纤激光器是一种新型的多波长光纤激光器,其原理是利用受激布里渊增益和掺铒光纤的线性增益,可以在常温下得到波长间隔约为0.08nm(~10GHz)的多波长输出。报道的布里渊掺铒光纤激光器,在布里渊抽运功率为1.7mW、980nm抽运功率为300mW的情况下得到稳定的15个波长(间隔~10GHz)的输出,这种激光器用作光传感器、光谱分析仪以及密集波分复用系统的光源。实验发现,输出波长的个数随着980nm抽运功率的增大而增加。另外,布里渊掺铒光纤激光器的信号功率主要来自于掺铒光纤的增益,而布里渊增益对它的影响不大。  相似文献   

7.
对光纤环形腔技术的传感原理进行了理论推导,并设计了一种双环路一氧化碳浓度测量系统.分析了掺铒光纤放大器在系统中的作用及其增益波动对系统的影响,通过对掺铒光纤放大器的增益进行反馈控制,进一步了提高了测量系统的稳定性和精确性.通过实验,得出了不同浓度的一氧化碳所对应的衰荡曲线.分析了不同浓度的气体对光的吸收特性及衰荡时间与浓度的关系,为实现气体浓度的高准确度在线测量提供了重要的依据.  相似文献   

8.
掺铒孔辅助导光光纤是由掺铒的高折射率纤芯、低折射率包层和少量的空气孔组成. 采用有限元法分析了掺铒孔辅助导光光纤的模式特性;给出了数值计算截止波长和模场直径的方法;提出了改进的平均粒子数反转度迭代算法来数值计算掺铒光纤放大器的增益和噪声系数. 研究空气孔对掺铒孔辅助导光光纤的截止波长、模场直径和放大器的增益系数的影响. 发现:减小相对孔芯距的值,可使截止波长向短波长移动,减小模场直径的值;当孔的相对大小较大时,截止波长、模场直径和增益的最大值基本上不随孔的相对大小的增大而改变. 最后,综合考虑掺铒光纤基模和二阶模的截止波长、与普通单模光纤的熔接损耗、放大器的增益和噪声系数等因素,优化设计了掺铒孔辅助导光光纤的四个结构参量——纤芯半径、纤芯与包层的折射率差、相对孔芯距和孔的相对大小. 关键词: 孔辅助导光光纤 掺铒光纤 光纤放大器 有限元法  相似文献   

9.
陈健  温扬敬 《光子学报》1998,27(5):396-401
分析了平均孤子传输系统中用于能量补偿的掺铒光纤放大器增益超过或低于理想值时平均孤子传输特性的劣化,提出并证明了利用工作在饱和区的掺铒光纤放大器可实现平均孤子在能量补偿偏离时自稳定传输,讨论了这一措施的可行性及适用范围。  相似文献   

10.
对1550 nm铒镱共掺光纤放大器不同温度下的输出功率以及经过高温老化后的输出功率和光谱进行了实验研究.通过对比高温和常温下铒镱共掺光纤放大器的输出功率随泵浦功率的变化曲线,得出铒镱共掺光纤放大器在高温环境工作可提高输出功率,且不同长度的增益光纤对温度的敏感性不同的结论.以Arrhenius模型为加速老化模型对增益光纤...  相似文献   

11.
The structure of combining two segments of erbium-doped fiber (EDF) together—one EDF acting as an amplifier and the other as an absorber—has a special gain characteristic curve which has a maximum gain with an increase in the input signal power. This special gain characteristic curve can lead to an optical bistability (OB) phenomenon in a fiber-ring laser employing an EDF of this structure. By adjusting the pump light power injected into the second segment of the EDF, we can change the behavior of the absorber and can, therefore, control the range of the bistability region. A method is proposed to calculate the tunable optical bistability, and the calculation result is in accordance with our experiment.  相似文献   

12.
We demonstrate a multi-wavelength erbium-doped fiber laser (EDFL) using erbium gain and four-wave mixing (FWM) effect in a piece of erbium-doped fiber (EDF) with high erbium ion concentration. The EDF has a pump absorption rate of 24.6 dB/m at 979 nm and is bi-directionally pumped by 980-nm laser diodes. FWM effect redistributes the energy of different oscillating lines and causes multi-wavelength operation. The laser generates more than 22 lines of optical comb with a line spacing of approximately 0.10 nm at the 1569-nm region using only 1.5-m-long EDF.  相似文献   

13.
We demonstrate a new optical bistability devise by using two Fiber Bragg Gratings (FBG), in which an erbium-doped fiber (EDF) is inserted to form a nonlinear Fabry–Perot cavity (EDF FBG/F–P). The operation principle of this device is described by the resonant nonlinearity theory combining with the transfer matrix method. The optical bistability behaviors under different parameters are investigated. It shows that EDF FBG/F–P device has an evident merit in reducing the threshold switching power to 7 mW, resulting in a reduction about 6 orders, compared with that of single FBG device. Moreover, the ultra-fast response time about 35 ps is also confirmed.  相似文献   

14.
从理论和实验上研究了带有高频二氧化碳激光写入的低成本长周期光纤光栅(LPFG)掺铒光纤放大器(EDFA).结果表明,单波长和多波长EDFA的性能都可以通过在掺铒光纤(EDF)中插入长周期光纤光栅用作自发辐射噪声(ASE)滤波器或增益平坦器来提高性能.优化设计了带LPFG噪声滤波器的线放EDFA,与没有LPFG噪声滤波器相比,线放的噪声和小信号增益分别被减小和提高了约0.5 dB和7 dB。通过在多波长EDFA的EDF中插入一个LPFG增益平坦滤波器的方法,获得了1.5 dB的增益平坦度,与没有LPFG平坦器相比,EDFA的噪声被减小了0.1 dB,增益被提高了1 dB.  相似文献   

15.
Optimization of gain flattened C-band erbium-doped fiber amplifier (EDFA) using a macrobending method with an improved gain flatness and bandwidth is demonstrated. The optimization for gain flatness and bandwidth was achieved by varying the bending radius and the length of the doped fiber. In the optimized condition, the gain saturation effect as well as the energy transfer from shorter wavelengths to longer wavelengths resulted in a flattened and broadened gain profile in the C-band region. The amplifier was optimized to a 9 m long erbium-doped fiber (EDF) with erbium ion concentration of 1100 ppm and bending radius of 6.5 mm. The gain variation of the EDFA is obtained within ±1 dB over 25 nm bandwidth of C-band region.  相似文献   

16.
We have been experimentally demonstrated an active control technique of dynamic gain-clamped spectra for the erbium-doped fiber amplifiers (EDFA's) by a backward-injected Fabry-Perot (F-P) laser into this EDFA. In addition, employing a short length erbium-doped fiber (EDF) that not cause any gain saturation for preamplification in front of this amplifier module, it can reduce the noise figure degradation and simultaneously achieve gain variation from 11.1 dB to 0.5 dB for 10 dB input power level change.  相似文献   

17.
光纤参变放大器光纤长度的优化设计   总被引:1,自引:1,他引:0  
曹辉  孙军强  张新亮  黄德修 《光学学报》2004,24(8):085-1090
随着高输出功率掺铒光纤放大器和高非线性光纤的出现和使用,光纤参变放大器(OPAs)中出现了越来越多的增益饱和现象,这是光放大器中应该尽量避免的。对此,提出了依据光纤参变放大器的光纤非线性系数、抽运光功率、信号输入功率等参量对光纤长度进行优化设计的解决思路。明确提出最佳光纤长度的概念,即在其他参量一定的情况下使信号增益或信号输出功率达到最大所需的最小光纤长度,而且最佳光纤长度有利于提高光纤参变放大的增益带宽和波长转换带宽。通过数值积分求解描述光纤参变放大过程的非线性耦合方程,并运用控制变量法深入研究了最佳光纤长度与光纤非线性系数、抽运光功率、信号输入功率的关系。最后用最小二乘法进行数据拟合确定系数,得到简洁、实用的最佳光纤长度解析表达式。与已有实验结果比较表明,该解析式可很好地用来计算和优化光纤参变放大的光纤长度。  相似文献   

18.
We present a stable linear-cavity single longitudinal mode (SLM) erbium-doped silica fiber laser. It consists of four fiber Bragg gratings (FBGs) directly written in a section of photosensitive erbium-doped fiber (EDF) to form asymmetric three-cavity structure. The stable SLM operation at a wavelength of 1545.112 nm with a 3-dB bandwidth of 0.012 nm and an optical signal-to-noise ratio (OSNR) of about 60 dB is verified experimentally. In laboratory condition, the performance of power fluctuation of less than 0.05 dB observed from the power meter for 6 h and wavelength variation of less than 0.01 nm obtained from the optical spectrum analyzer (OSA) for about 1.5 h are demonstrated. The gain fiber length is no longer limited to only several centimeters for SLM operation because of the excellent mode-selecting ability of the asymmetric three-cavity structure. The proposed scheme provides a simple and cost-effective approach to realizing a stable SLM fiber laser.  相似文献   

19.
We experimentally investigate the gain saturation effect of a piece of 8 m long Erbium doped fiber (EDF), we introduce a theoretical model for the EDF ring loop, and our simulation results show very good cross-gain modulation (XGM) and wavelength conversion. We also experimentally investigate the XGM in an EDF ring loop system. Based on the study of the XGM in the EDF ring loop system, a wavelength conversion is designed with the EDF ring loop system. The EDF ring loop systems as a wavelength conversion is experimentally demonstrated by converting a sinusoidal modulated optical signal at wavelength of 1551 nm to an optical signal at wavelength of 1553.3 nm.  相似文献   

20.
长波段掺铒光纤放大器用掺铒光纤的设计考虑   总被引:2,自引:0,他引:2  
罗杰  叶培大  伍叔坚  程淑玲 《光子学报》2000,29(12):1138-1141
本文分析了长波段掺铒光纤放大器(EDFA)的增益系数与Er3+离子浓度的关系.研制了铝共掺杂的高浓度掺铒光纤,以缩短长波段掺铒光纤的长度.用两级泵浦实现了L-波段EDFA.光纤放大器的掺铒光纤总长18m,在1570nm波长处的小信号增益为42.26dB,输出功率为17.5dBm.我们认为,较低的浓度淬灭效应归因于光纤中较高的A1掺杂浓度.当总的输入信号功率为-3dBm时,在1570至1600nm间的7路WDM信号的增益不平坦度仅为0.68dB..  相似文献   

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