共查询到20条相似文献,搜索用时 78 毫秒
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利用全量子理论和多模受激拉曼散射模型,研究了拉曼放大中,考虑泵浦光耗散时,斯托克斯光和泵浦光二阶量子关联函数随相互作用距离变化的特性,在不计及色散的影响时,斯托克斯光和泵浦光的二阶量子关联函数的变化主要取决于输入斯托克斯光和泵浦光的光强比,在极限情况下,本文的计算结果与拉曼产生的计算结果和经典耦合波理论的计算结果相符合。 相似文献
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泵浦光束质量对受激拉曼散射的影响 总被引:3,自引:3,他引:0
主要讨论泵浦光束质量对低气压拉曼种子源特性的影响。文中给出了一阶斯托克斯光泵浦阈值、输出能量和光束质量的实验数据。用M^2因子分析了泵浦光和一阶斯托克斯光的光束质量。根据考虑泵浦聚焦和泵浦光束质量影响的近似拉曼散射理论计算了泵浦阈值的理论曲线,并与实验数据和有关文献进行了比较。 相似文献
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序列脉冲倍频YAG激光器泵浦的氧气受激拉曼散射研究 总被引:2,自引:2,他引:0
对序列脉冲倍频YAG激光器泵浦的氧气受激拉曼散射进行了研究。对氧气的受激拉曼散射池的热传导过程进行了数值模拟计算,实验研究了序列脉冲倍频YAG激光器泵浦情况下氧气受激拉曼散射的热效应问题。 相似文献
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在有损耗、色散和自相位调制的影响下,通过分段分析法计算了自发拉曼散射光子的二阶相关函数,研究了长光纤中脉冲光泵浦下自发拉曼散射的时间模式特性。研究结果表明:在无色散和自相位调制的情况下,自发拉曼散射光子的二阶相关函数不受泵浦光损耗的影响,仅由泵浦光脉宽和拉曼光子相干时间之间的比值决定,与自发参量下转换光子的二阶相关函数具有相同的表达式;在有色散和自相位调制的情况下,由色散和自相位调制共同引起的泵浦光脉宽变化,以及泵浦光和拉曼光子间色散致走离,使拉曼光子的时间模式发生改变。自发拉曼散射光子的二阶相关函数取决于光纤损耗系数、色散参数和初始泵浦光脉宽等因素,不再与自发参量下的转换光子相同。 相似文献
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介绍了一种将反向传播(BP)神经网络算法与人工蜂群算法相结合的方法,并用该方法对多泵浦拉曼光纤放大器的设计进行了优化.通过研究多层BP神经网络中的隐藏层层数和神经节点数,确定了最佳的学习模型,该模型可以精准地反映泵浦波长和泵浦功率与拉曼净增益分布间的映射关系,能代替传统求解拉曼耦合波方程的方法.同时,为了提高增益谱的平坦性,采用人工蜂群算法来优化泵浦参数,得到了最优的泵浦波长和泵浦功率.仿真结果表明,通过将训练好的BP神经网络模型加入到人工蜂群算法中,所研究的拉曼放大器达到了期望的增益性能,且其目标值与预测值的最大误差不超过0.29 dB.该设计方案为拉曼光纤放大器的研究提供了新的思路和方法. 相似文献
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Masahiro Ikeda 《Optics Communications》1981,39(3):148-152
Spectral Raman amplification characteristics have been measured directly for a tunable pumping source, taking the relative polarization states of pump and signal waves into consideration. Raman amplification has been observed, even with an orthogonal polarization pump, in a long span single mode fiber. Raman amplification causes significant crosstalk in wave-length-multiplexed systems. 相似文献
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同时考虑接收光信噪比(OSNR)及非线性失真影响,对分布式光纤拉曼放大器在长距离光传输系统中的最优抽运方式进行了研究.利用变分法原理获得了在不记双瑞利背散射(DRB)影响时的最优信号功率分布函数——均匀分布,但考虑双瑞利散射影响时则不存在解析的最优分布函数.在分别考虑长、短光纤跨距的情况下,比较了三种具有代表性的分布式光纤拉曼放大方式,即双向二阶拉曼抽运、双向一阶拉曼抽运和拉曼+掺铒光纤放大器混合放大方式的性能.指出通过优化一阶抽运波长以及一阶到二阶抽运功率比,对称结构的双向二阶抽运在绝大部分情况下可以在
关键词:
光纤拉曼放大器
双瑞利背散射
变分法
光纤非线性 相似文献
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L. Gruner-Nielsen Y. Qian P.B. Gaarde 《Journal of Optical and Fiber Communications Reports》2006,3(2):61-89
Dispersion compensating fibers (DCF) are the most widely used technology for
dispersion compensation. A DCF without Raman amplification introduces extra
loss in the system, thus increasing the need for gain in the discrete
amplifiers and degrading the noise performance. The idea to additionally use
the DCF as a Raman gain medium was originally proposed by Hansen et al. in
1998. [1] This was quickly followed by Emori et al., who
demonstrated a broadband, loss less DCF using multiple-wavelength Raman
pumping. [2] DCF is a good Raman gain medium, due to a
relatively high germanium doping level and a small effective area. To get
sufficient gain with a reasonable pump power, a discrete Raman amplifier has
to contain several kilometers of fiber, adding extra dispersion to the
system that must be handled in the overall dispersion management. Dispersion
compensating Raman amplifiers integrates two key functions: dispersion
compensation and discrete Raman amplification into a single component. 相似文献
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In a distributed Raman fiber amplifier (DRFA), Raman amplification allows a lower signal launch powers to transverse the span above the noise floor while still increasing the optical signal-to-noise ratio (OSNR). It improves the noise figure and reduces the nonlinear penalty of fiber systems. In this paper, we demonstrate a new trend of OSNR at different pump configurations: forward, backward and bidirectional pumping for DRFAs as a function of fiber length. We also present the variation of OSNR with both input pump power and input signal power. It is found that forward pumping provides the highest OSNR, reaching its maximum value of 37 dB. However, backward pumping provides the smallest OSNR that has its maximum of 22 dB and the bidirectional pumping provides the moderate OSNR between the others having its peak of 26 dB. 相似文献
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We present a vector theory of Raman amplification and use it to discuss the effect of polarization-mode dispersion (PMD) on the Raman gain process inside the optical fiber used for stimulated Raman scattering. We show that the PMD induces large fluctuations in the amplified signal and reduces the average value of the amplifier gain. In the case of forward pumping, fluctuations are expected to be more than 15% under typical operating conditions and can exceed 50% for fiber with a relatively low value of the PMD parameter. The PMD effects are much less severe in the case of backward pumping. Signal fluctuations reduce to less than 1% in this case when the PMD parameter exceeds 0.05 ps/ radicalkm. 相似文献
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1410 nm波段分布式光纤拉曼增益放大器的研究 总被引:6,自引:2,他引:4
讨论了分布式光纤拉曼增益放大器的工作原理,采用1320nm固体激光器作为抽运源,获得了1410nm波段附近的光放大,在单模GI光纤长度为23km时,初步研究了拉曼放大器增益与光纤作用长度的关系,抽运脉冲峰值功率分别为50W、30W时,光纤的有效作用长度分别为15.5km和10.5km;研究了在不同的光纤有效作用长度时,拉曼放大器增益与抽运功率的关系;从光纤拉曼光谱图估算了光纤拉曼放大器的光谱宽度为50nm或250cm^-1。 相似文献
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The probe gain with and without inversion in a four—level atomic model:light amplification at a short wavelength 下载免费PDF全文
We propose a new four-level atomic model for achieving light
amplification at a short wavelength, where direct incoherent
pumping into the top level is avoided by the advantage of
coherent pumping. In this model, the lower level of the probe
transition is an excited state but not the usual ground state.
By analytical as well as numerical calculations, we find that the
probe gain, either with or without population inversion, which depends
on the relation between spontaneous decay rates $\g_{42}$ and $\g_{21}$, can be achieved with proper parameters. We note that the Raman scattering
gain always plays an important role in achieving the probe amplification. 相似文献
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We report a steady-state Raman gain measurement of the Q(1)(0) transition (v = 1 ? 0, J = 0 ? 0) in solid parahydrogen. We carry out measurements by pumping with a continuous-wave frequency-doubled YAG laser at 532 nm and observing the direct amplification of a probe-laser beam for the first Stokes transition at 683 nm. A large single-pass amplification coefficient of 2.3 +/- 0.2 is obtained at a pump intensity of 46 kW/cm(2), with an interaction length of 1 cm, giving a steady-state Raman gain coefficient of 18 +/- 3 cm/MW. 相似文献
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Here we summarize multi-terabit long-haul transmission experiment and distributed Raman amplification (DRA) technologies. As well, we investigate the configuration of dispersion-managed fibers for the DRA-based system from the viewpoint of the fiber non-linear effect and required pumping power. 相似文献
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An L-band remotely-pumped erbium-doped fiber amplifier incorporating a secondary pumping scheme utilizing stimulated Raman
Scattering (SRS) was demonstrated. 1423 nm Raman laser was employed to generate SRS which became the secondary pump source.
The amplifier displayed excellent gain of up to 27.3 dB at 1570 nm for −30 dBm input. Noise figures were also kept to a minimum,
with the highest figure measured at 11 dB which was influenced by imperfection of the C/L coupler utilized in this architecture.
Overall transmission performance was measured as well and demonstrated an encouraging outcome with gain as high as 24 dB while
the noise figure was maintained at about 11 dB. The L-band signal amplification was also contributed by the stimulated Raman
scattering along the transmission fiber. The outcome of this study emphasized the feasibility of secondary pumping scheme
using SRS in L-band gain enhancement. 相似文献