共查询到16条相似文献,搜索用时 109 毫秒
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色散渐减光纤组成的环形镜对高阶孤子的理想压缩 总被引:6,自引:6,他引:0
利用数值模拟方法证明,采用色散渐减光纤组成的非线性光纤环形镜不仅可压缩高阶光孤子,而且能有效地消除压缩后脉冲的底座、提高光脉冲的输出能量.研究表明,对于一确定的色散渐减光纤,只要选取不同环形镜长度,即可对不同阶数的高阶孤子进行理想压缩.且孤子阶数越高,所需最佳环形镜长度越短、压缩后光脉冲的峰值强度越大、能量透射率越低.研究同时发现,环形镜的功率分束比存在一最佳值,在此值下所得压缩后的光脉冲不仅具有较大的峰值及能量透射率,且不含底座. 相似文献
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单模光纤中基于暗孤子交叉相位调制的亮脉冲压缩 总被引:9,自引:2,他引:7
对单模光纤正群速色散区中基于暗孤子交叉相位调制的亮脉冲压缩进行了定量计算和详细分析,结果表明,亮脉冲的压缩程度与昱孤子相对于亮脉冲的初始峰值功率有关,初始相对峰值功率愈高,亮脉冲的压缩比和压后的峰值功率愈高,同时所需的光纤长度愈短,对于给定的初始条件,光纤长度存在一最佳值,在最佳长度处,压缩后的亮脉冲峰值功率最高,宽度最窄。 相似文献
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色散缓变光纤中飞秒高阶孤子脉冲的增强压缩 总被引:6,自引:4,他引:2
提出了一种利用孤子绝热放大效应与高阶孤子脉冲压缩效应相结合来压缩飞秒高阶孤子的新方法.通过数值模拟方法证明,采用三阶色散为负的色散缓变光纤压缩高阶孤子,可利用喇曼散射效应与负三阶色散的相互作用,消除正三阶色散对光脉冲压缩产生的不利影响,增加压缩比,提高压缩后光脉冲的质量.研究表明,在色散缓变参量一定的情况下,孤子阶数越高,所需最佳光纤长度越短、光脉冲的压缩比越大;对于相同功率的孤子光脉冲,光脉冲的压缩比随着色散缓变参量的增大而增大;无论是孤子脉冲还是高斯脉冲都适合于色散缓变光纤中的高阶孤子脉冲压缩. 相似文献
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根据超短光脉冲在光纤中传输的非线性薛定谔方程,模拟了不同色散参量情况下色散补偿和色散位移光纤对增益开关半导体激光器产生的光脉冲的压缩,给出了光脉冲在经过色散补偿光纤前后的啁啾曲线。结果表明,使用色散参量D分别为-150,-180和-20ps/(nm·km)的色散补偿光纤可以实现其他脉冲压缩方法的压缩效果,最大压缩因子达到6.09,但色散参量越大,所需光纤长度就越短。此外,脉冲经过色散补偿光纤后线性啁啾几乎为零。还利用色散位移光纤对脉冲进行孤子压缩,脉冲宽度由最初的45ps减小到1.23ps。指出采用这2种光纤相结合的方法可以对光脉冲实现高效压缩。 相似文献
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光纤损耗对皮秒脉冲孤子效应压缩的影响 总被引:16,自引:2,他引:14
在计及常规光纤损耗的前提下,通过数值求解求解修正的非线性薛定谔方程,全面地计算和分析了损耗对皮秒脉冲在单模光纤中孤子效应压缩过程的影响。结果表明,与不计及损耗时相比,损耗一方面导致脉冲压缩比,压缩后的脉冲峰值功率和脉冲压缩质量的下降,另一方面还导致所选用的最佳光纤度的增加。进一步研究表明,损耗对脉冲压缩的影响程度还与输入脉冲的峰值功率和脉宽有关。 相似文献
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脉冲离散效应对光纤中基于交叉相位调制的脉冲压缩的影响 总被引:4,自引:1,他引:3
通过数值模拟,分析了脉冲离散效应对单模光纤正群速色区基于暗孤子交叉不相位调制的脉冲压缩的影响,并提出了减轻这种影响的办法,作者发现,即使暗孤子与被压缩脉冲的中心波长相差很小,离散效应对脉冲压缩的影响也很大,离散效应不仅导致脉冲压缩比的减小和压缩后脉冲峰值功率的降低,而且还导致脉冲压缩所需最佳光纤长度的增加以及压缩后的脉冲呈现不对称性,还发现,若采取本文提出了的非同步耦合法,则可以明显地弥补离散效应 相似文献
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Huifang Ma Xia Zhang Qi Jing Yongqing Huang Xiaomin Ren 《Optics & Laser Technology》2012,44(5):1333-1337
In this paper, enhancement of bandwidth of supercontinuum generated in a normal dispersion-flattened microstructured fiber by using compressed pulse is demonstrated experimentally and numerically. Using high-order soliton compression effect, the standard single mode fiber is used as a pulse compressor. The experimental measured ?10 dB spectral width is broadened from 75 nm to more than 140 nm by adding a 20 m long standard single mode fiber. Numerical analysis shows that using pulse compressed by a certain length fiber can increase the spectral bandwidth without making extra amplitude noise. 相似文献
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In this paper, four common dispersion profiles have been investigated for obtaining as high as possible wings free compressed pulse in nonlinear fiber loop mirror. Results show that linear profile can be considered as the best choice. Also, as the importance for enhanced adjustability of higher order soliton effect pulse compression, we propose a new simple method, as active fiber loop. According to our investigation it can be seen that when the amplification factor changes from 3 dB to 4 dB in an active linear profile dispersion decreased fiber loop mirror, the compression factor can be adjusted to any desired value between 140 and 170 where it is approximately two times higher than passive loop. 相似文献
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Obulkasim Oluk Bai-Song Xie Muhmmad Ali Bake Sayipjamal Dulat 《Frontiers of Physics》2014,9(2):157-163
By solving the quantum Vlasov equation, electron positron pair production in a strong electric field with asymmetric laser pulses has been investigated. We consider three different situations of subcycle, cycle and supercycle laser pulses. It is found that in asymmetric laser pulse field, i.e.. when the pulse length of one rising or falling side is fixed while the pulse length of the other side is changed, the pair production rate and mnnber density can be significantly modified comparable to symmetric situation. For each ca,se of these three different cycle pulses, when one side pulse length is constant and the other side pulse length becomes shorter, i.e., the whole pulse is compressed, the more pairs can be produced than that in tile vice versa case, i.e., the whole pulse is elongated. In compressed pulse case there exists an optimum pulse length ratio of asylnmetric pulse lengths which makes the pair number density maximunn. Moreover, the created maximum pair number density by subcycle pulse is larger than that by cycle or/and supercycle pulse. In elongated pulse case, however, only for supercycle laser pulse the created pairs is enhanced and there exists also an optimum asymmetric pulse length ratio that maximizes the pair number density. On the other hand. surprisingly, in both cases of subcycle and cycle elongated laser pulses, the pair number density is monotonically decreasing as the asymmetry of pulse increases. 相似文献