飞秒光脉冲基于交叉相位调制的压缩脉冲对的产生

数值模拟了在喇曼散射效应影响下,波长位于反常色散区的高阶孤子泵浦脉冲与波长在正常色散区的信号脉冲通过交叉相位调制作用产生的压缩脉冲对.结果表明,由于受喇曼效应的影响,飞秒信号脉冲产生的脉冲对不再保持对称,滞后的蓝移脉冲峰值功率随传输距离的增加而减小,产生孤子红移.同时发现喇曼系数增大,超前红移脉冲峰值功率增加,滞后蓝移脉冲峰值功率降低.分析了孤子阶数和正、负走离效应对脉冲压缩对变化规律的影响.     

飞秒光脉冲基于交叉相位调制的压缩脉冲对的产生

数值模拟了在喇曼散射效应影响下,波长位于反常色散区的高阶孤子泵浦脉冲与波长在正常色散区的信号脉冲通过交叉相位调制作用产生的压缩脉冲对.结果表明,由于受喇曼效应的影响,飞秒信号脉冲产生的脉冲对不再保持对称,滞后的蓝移脉冲峰值功率随传输距离的增加而减小,产生孤子红移.同时发现喇曼系数增大,超前红移脉冲峰值功率增加,滞后蓝移脉冲峰值功率降低.分析了孤子阶数和正、负走离效应对脉冲压缩对变化规律的影响.     

光孤子脉冲在光纤放大器中的传播

本文建立了包括增益色散,受激喇曼散射,双光子吸收效应的理论模型,讨论了光孤子脉冲在光纤放大器中的传播.数值计算结果表明:在反常色散范围内,光孤子的放大是不稳定的.增益色散导致光脉冲对称分裂,而受激喇曼散射则导致不对称的分裂.在增益色散和受激喇曼散射的共同作用下可获得新的时域和频域特征.有限带宽的放大能抑制受激喇曼散射引起的自频移.本文对有啁啾的光孤子脉冲的放大也进行了分析.     

光通信 光传输、通信理论

TN911 2006032509偏振模色散对飞秒孤子脉冲传输的影响=Influence of po-larization mode dispersion on femtosecond optical solitontransmission[刊,中]/李志全(燕山大学电气工程学院.河北,秦皇岛(066004)) ,阎利娟…∥光电子技术与信息.—2006 ,19(2) .—40-43以Maxwell电磁场理论为基础,在综合考虑了高阶色散、高阶非线性、自相位调制、交叉相位调制、自变陡、脉冲内喇曼散射以及偏振模色散(PMD)等因素的基础上,推导了飞秒孤子脉冲在双折射光纤中传输的耦合非线性薛定谔方程(NLSE)。利用分步傅立叶方法对该方程进行了数值计算,通…     

单模光纤中受激喇曼散射对调制不稳定性的影响

基于修正的非线性薛定谔方程，利用线性扰动理论和数值方法研究了单模光纤中的调制不稳定性.由于受激喇曼散射的作用，使得喇曼增益谱叠加到光纤中的调制不稳定性增益谱上.这样，原本调制稳定的光纤正常色散区也出现了调制不稳定性；而在反常色散区，随着初始功率的增加，常规的调制不稳定性增益谱的增益和频谱范围均增大，而喇曼增益谱的增益增大但其频谱范围基本不变，这样导致常规的不稳定区域逐渐侵入并最终掩盖喇曼增益区.数值模拟验证了解析结果的正确性，并证明了利用反常色散情形下的调制不稳定性可以产生超短脉冲序列，但这种脉冲序列的进一步传输将会出现喇曼孤子自频移现象.     

分布式EDFA中受激喇曼散射对光孤子脉冲传输的影响

本文用数值方法研究了透明传输下,受激喇曼散射(SRS)对由分布式掺饵光纤放大器(d-EDFA)级联的传输线中传输的光孤子脉冲的泵功率、孤子脉冲平均功率演化、均方根脉宽谱宽积、孤子系统的能量辐射、以及对光孤子传输稳定性的影响.结果表明:SRS降低了系功率,减弱了孤子平均功率起伏,有利于光孤子传输,但也使孤子脉(谱)宽展宽,增大了孤子系统的能量辐射,对孤子传输稳定性产生不良的影响.     

光纤中强受激喇曼散射时的自相位调制

在光纤-光栅对激光脉冲压缩中,由于受激喇曼散射和自相位调制的竞争,使得泵浦激光脉冲波形重整,且自相位调制谱极不对称。本文用2m的单模保偏光纤,在产生较强的受激喇曼散射的情况下,得到较为对称的泵浦激光的自相位调制功率谱,并讨论了自相位调制功率谱的一些特点。     

飞秒光纤激光器

我们利用同步泵浦光纤喇曼环形激光器在1.396μm处得到195fs 的光脉冲,并利用时间-色散调谐技术在1.396μm附近实现了47nm 的波长调谐.我们采用1.313μm的 Nd:YLF 锁模脉冲泵浦,其喇曼光处于单模光纤的负色散区,利用孤子效应得到195fs 的光脉冲.实验中我们采用一台 Nd:YLF(Quantronix Model 4216d)激光器作泵浦源,输出波长为1.313μm,主动锁模时输出脉宽约50ps.泵浦光经一枚双色镜反射后耦合进光纤.测试中使用的单模光纤是普通通讯用单模石英光纤.其零色散波长在1.305μm,芯径约为9.5μm.由于喇曼效应的作用,在光纤中产生1.395μm左右的喇曼光.喇曼光从光纤出来后经透镜准直、延迟后穿过双色镜反馈回光纤,其中一部分被反射作为输出.用 PIN 来监测泵浦脉冲与喇曼光脉冲的同步情况,并调节延迟线达到同步泵浦的要求.     

光纤中的受激喇曼散射及泵浦脉冲和斯托克斯脉冲的分离

本文报道在单模光纤中的受激喇曼散射的实验结果,用条纹相机测量了泵浦脉冲和喇曼斯托克斯脉冲时间上的相对延迟;结果表明,受激喇曼散射的喇曼斯托克斯脉冲大约在距光纤输入端一个分离距离的位置上形成。     

高功率纳秒光脉冲在单模光纤中的受激喇曼散射及抑制研究

利用包含喇曼增益、抽运消耗、自相位调制、交叉相位调制和群速度色散效应的耦合非线性薛定谔方程组,对千瓦级高功率纳秒脉冲在单模光纤中的传输特性进行了模拟计算.分析了输入脉冲和斯托克斯脉冲的演化过程,研究了大模面积光纤对受激喇曼散射的抑制作用.研究结果表明,采用模面积为530 μm~2的光子晶体光纤作为惯性约束聚变脉冲整形系统的传输介质,能有效抑制受激拉曼散射,不但信号衰减较小,而且中心凹陷程度较低.     

Generation of a stationary train of chaotic soliton-like microwave pulses in self-oscillating ring systems with a ferromagnetic thin film

The generation of a stationary train of chaotic soliton-like microwave pulses has been observed in an isolated self-oscillating ring system with a ferromagnetic thin-film and a resonator. The pulses have been formed owing to three-wave parametric processes and modulation instability of a surface magnetostatic wave. The soliton-like character of the microwave pulses is indicated by the time dependence of the instantaneous phase of the signal envelope.     

Nonlinear focusing of picosecond baseband pulses in paraelectric crystals

The nonlinear baseband electromagnetic pulses of a wide spectrum that lies in terahertz (THz) range are investigated theoretically in the paraelectric crystals like SrTiO₃ at the temperatures ~ 77 K. The frequency dispersion is important in THz range there. The dominating nonlinearity of the crystal is cubic. The frequency dispersion and nonlinearity correspond to existence of envelope solitons and the modulation instability of long input envelope pulses, whereas in the transverse direction the modulation instability is absent. When the nonlinear wave is uniform in the transverse direction, the existence of soliton-like baseband pulses without a carrier frequency has been demonstrated. There exists a possibility to generate the regular sequences of short baseband pulses due to the nonlinearity in the paraelectric crystals. The nonlinear focusing of input long baseband pulses by the exciting antenna results in the formation of extremely short baseband pulses localized both in the longitudinal and transverse directions.     

Nonlinear dynamics of a pulse in an anisotropic medium with birefringence

The dynamics of a wave packet propagating in an anisotropic nonlinear optical fiber with strong linear coupling of the orthogonal components of the pulse is studied. The regimes of modulation instability and formation of soliton-like pulses are analyzed for different polarization angles of the incident light with allowance made for the first-and second-order dispersion effects and the nonlinear effects of self-and cross-modulation.     

Stability of chirped bright and dark soliton-like solutions of the cubic complex Ginzburg-Landau equation with variable coefficients

We consider an inhomogeneous optical fiber system described by the generalized cubic complex Ginzburg-Landau (CGL) equation with varying dispersion, nonlinearity, gain (loss), nonlinear gain (absorption) and the effect of spectral limitation. Exact chirped bright and dark soliton-like solutions of the CGL equation were found by using a suitable ansatz. Furthermore, we analyze the features of the solitons and consider the problem of stability of these soliton-like solutions under finite initial perturbations. It is shown by extensive numerical simulations that both bright and dark soliton-like solutions are stable in an inhomogeneous fiber system. Finally, the interaction between two chirped bright and dark soliton-like pulses is investigated numerically.     

Soliton—Like Pulses in Vertical Granular Chain Under Gravity：Particle—Like or Wave—Like

We numerically study the propagation,reflection and collision of soliton-like pulses in the vertical granular chain under gravity.For the pure granular chain system,during the propagation and reflection preocesses at the fixed end ,it behaves like a particle .When it is reflected at the free end ,it behaves as neither particle-like nor wave-like.When the stengths of the two colliding soliton-likie pulses are close,they collide just like particles.When their strengths are greatly different,they collide just like waves.For the soliton behavior in the collision process,from particle-like to wave-like,there is a critical value c for the ratio of the strengths of the two initial pulses.For the two-layer granular chain,if the mass of the grains in the second layer is less than that in the first layer,the soliton-like pulse in the first layer usually excites about[1/m]soliton-like pulses in the second layer.     

Nonparaxial propagation of soliton-like laser beams-pulses in media with saturable nonlinearity

The theoretical analysis of manifestations of nonparaxiality of propagation (in the plane transverse to the direction of propagation of radiation) of soliton-like beams-pulses in self-focusing media with electronic saturable nonlinearity is carried out. It is shown that, in formation of such structures by pulses of a comparatively small duration, a modulation of the radiation intensity arises, which can result in a fragmentation of the beam in the longitudinal direction. The number and depth of such "jags" are governed by the power of the nonparaxial beam.     

Multifrequency parametric infrared Raman generation in KGd(WO(4))(2) crystal with biharmonic ultrashort-pulse pumping

Mutlifrequency parametric Raman generation was carried out in a KGd(WO(4))(2) crystal by use of a dual-wavelength Ti:sapphire laser system. It was found that with femtosecond pump pulses the efficiency of Raman generation is low because of the onset of self-phase modulation. The mechanism for suppression of stimulated Raman scattering by self-phase modulation is discussed. Employing 2-ps-long chirped pulses generated four Stokes and one anti-Stokes component.     

Generation of a sequence of frequency-modulated pulses in longitudinally inhomogeneous optical waveguides

The conditions for the generation and efficient amplification of frequency-modulated soliton-like wave packets in longitudinally inhomogeneous active optical waveguides have been studied. The possibility of forming a sequence of pico- and subpicosecond pulses from quasi-continuous radiation in active and passive optical waveguides with the group-velocity dispersion (GVD) changing over the waveguide length is considered. The behavior of a wave packet in the well-developed phase of modulation instability with a change in the waveguide inhomogeneity parameters has been investigated based on the numerical analysis.     

Dynamics of two-mode radiation in optical waveguides with strong mode coupling

Amplitude equations, as well as the effective dispersion and nonlinearity parameters, which define the dynamics of a wave packet formed by two strongly coupled modes, are derived with allowance for the frequency dependence of the linear mode coupling coefficient. These equations are used to study the onset of the modulation instability of the two-mode wave packet, soliton-like pulses, and compression modes. Unlike single-mode systems, the last two effects in optical waveguides may arise for both a negative and positive disper-sion of the waveguide material.     

Numerical Analysis of Induced Phase Modulation between Two Ultrashort Pulses in Silica Fiber by the Extended Finite-Difference Time-Domain Method

We have analyzed the induced phase modulation (IPM) for ultrashort (74 fs) two-pulse propagation in a silica fiber by the extended finite-difference time-domain (FDTD) method, considering all exact Sellmeier-fitting values and nonlinear polarization P_NL involving the Raman response function. We show that nonlinear polarization causes several phenomena in spectral characteristics of propagated pulses, such as self-phase modulation (SPM), self-steepening, Raman response and IPM, by the extended FDTD method. To the best of our knowledge, this is the first IPM calculation by the extended FDTD method for the simultaneous propagation of two ultrashort (74 fs) laser pulses in a silica fiber.