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      色散波长
相关语句
  dispersion point
     The Evolution of Chirp Near the Zero Dispersion Point in the Region of Anomalous Dispersion in Monomode Optical Fibers
     单模光纤反常色散区零色散波长附近的啁啾演变
短句来源
     Modulational instability of femtosecond optical pulses in fibers near zero dispersion point is investigated using an extended Schrodinger equation.
     利用修正的非线性Schrodinger方程研究了单模光纤中在最小群速度色散波长附近的调制不稳定性。
短句来源
     using numerical method,we simulate the evolution of chirp near the zero dispersion point when the dispersion interacts with nonlinear effect.
     利用数值方法,模拟了零色散波长附近群速度色散效应与自相位调制效应共同作用时啁啾的演变。
短句来源
      The relation between the dispersion and the loss for optical pulse propagating without distortion near the zero dispersion point in the fiber with slowly decreasing dispersion is obtained by means of an extended nonlinear Schrodinger equatiton. Modulational instability in the fiber with slowly decreasing dispersion is analyzed. Because of the fourthorder dispersion,modulational instability is still existed when secondorder dispersion equals to zero.
     利用准非线性薛定谔方程,得出在零色散波长处光脉冲在色散缓变光纤里无畸变传输所满足的色散和损耗的关系.分析了色散缓变光纤调制不稳定性,由于四阶色散的存在,在二阶色散等于零时,仍然存在调制不稳定性.并对比了色散缓变光纤和理想光纤的调制不稳定性增益谱
短句来源
  “色散波长”译为未确定词的双语例句
     In this article,a highly nonlinear photonic crystal fiber with a pure silica core is designed and fabricated,of which the core diameter is 1.65μm,the air hole diameter 4.75μm,the space between the hole centers 5.35μm,the zero dispersion wavelength 1 120 nm and the dispersion at wavelength of 800 nm-88 ps/(nm.km).
     文章作者设计并制造了一种纯硅芯高非线性光子晶体光纤,该光纤纤芯直径为1.65μm,空气微孔直径为4.75μm,孔中心间距为5.35μm,零色散波长为1120 nm,800 nm波长的色散为-88 ps/(nm.km)。
短句来源
     In the λ>1. 55μm dispersion-shift fibre,the amplification period of dark solitons is as twice as bright soliton's.
     对于零色散波长大于1.55μm的色散移位光纤,暗孤子的放大周期比亮孤子的放大周期大一倍。
短句来源
     The value of material dispersion is small and its slope is flatwhen the wavelength is longer than 1.6μm. The zero material dispersionwavelength λ_0 is 1.65μm and 1.69μm respectively.
     两种材料的色散参数曲线在大于1.6μm后很平缓,色散参数值也较小,零色散波长值分别为1.65μm和1.69μm。
短句来源
     Measurement and calculation of zero dispersion wavelength in infra-red fiber
     红外光纤零色散波长的测量和计算
短句来源
     The Measurement and Calculation of Zero Dispersion Wavelength in Infra-red Fiber
     红外光纤零色散波长的测量和计算
短句来源
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  相似匹配句对
     Measurement and Calculation of Zero Diapersion Wavelength
     零色散波长的测量与计算
短句来源
     Accurate Measurement of Zero Dispersion Wavelength in an Optical Fiber
     光纤零色散波长的精确测量
短句来源
     CHROMATIC DISPERSION IN FIBER OPTICS
     光纤的色散
短句来源
     THE DISCUSSION OF THE DISPERSION INTERACTION ENERGY
     色散力的探讨
短句来源
     The montoring wavelength was changed.
     变换波长检测;
短句来源
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  dispersion point
We discuss the effect of amplification of the signal wave for its frequency-degenerate two-wave interaction with pumping, when the field frequency is tuned to the "zero dispersion" point.
例句来源      
A dispersion-shifted SM fiber that has the zero dispersion point near the 1550-nm window, but outside the actual window used to transmit signals.
例句来源      
Furthermore the dispersion analysis gives a better idea of the behavior of each scheme from the dispersion point of view.
例句来源      
Meanwhile, the first zero dispersion point remains unchanged and the third zero dispersion point gradually shifted to the lower wavelength.
例句来源      
Most of the optical fiber utilized world-wide is nondispersion shifted fiber, with its zero dispersion point near 1.3 m.
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         A wideband nonlinear scattering spectrum (1.1—1.9 um) is obtained in a multimodeoptical fiber pumped with an A-O Q-switched Nd:YAG laser at 1.06 um.The spectrum forms a goodquasicontinuum at the zero-material-dispersion range of the fiber.Discussion about the generationmechanism of the continuum is given.It shows that the continuum is generated by combined interac-tion of stimulated Raman scattering and four-photon mixing.
            利用1.06μm声光调Q激光器作泵浦源,从多模光纤获得了光谱范围从1.1~1.9μm 的宽带非线性散射谱。散射谱在光纤零色散波长附近有较平坦的宽带准连续谱。我们认为此光连续谱是由受激喇曼散射与四光子混频过程的组合作用产生的。
文摘来源
         The zero dispersion wavelength of CsCl-type crystal is calculated under tight-binding approximation, with Coulomb interaction between the electron and the hole at the nearest neighbouring sites taken into account. It is shown that the material system can be looked upon as an ensemble of a series of polarization wave oscillators when we deal with the interaction of light and matter. The strengths of the polarization wave oscillator are calculated. The material dispersion and the zero dispersion wavelengths f...
            本文从微观参数出发,计算了氯化铯型离子晶体的零色散波长。我们利用二能带模型,在紧束缚近似下,仅考虑最近邻导带电子和价带空穴之间的库仑相互作用,求得了计算氯化铯型离子晶体色散参数的表达式和零色散波长的计算公式。讨论了氯化铯型离子晶体束缚激子的结合能、极化波振子强度、零色散波长和微观参数之间的关系。
文摘来源
         The chromatic dispersion measurement using phase shift technique is discussed In this paper. The spectral dispersion of single-mode fiber is measured and the zero chromatic dispersion wavelength, the slope of dispersion vs. wavelength are obtained. The chromatic dispersion of multimode fiber is also measured. The theoretical analysis of its accuracy is presented in the paper and the influence of random noise to phase shift measurement is calculated.The chromatic dispersion measurements have been carried on ...
            本文讨论了采用相移法测量光纤色度色散的技术。对单模光纤的色散谱进行测量,得出单模光纤的零色散波长和色度色散波长变化的斜率。此外,还对多模光纤的色度色散进行了测量。本文对测量精度作了理论分析,计算了随机噪声对相移测量的影响。 分别在二个波长区域——短波长区域(0.85μm附近)和长波长区域(1.3μm附近)对多模光纤和单模光纤的色度色散进行了测量,所得结果与用其它方法所测得的结果符合良好。
文摘来源
 
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