1) zero dispersion
零色散
1.
Efforts are also made to study the possibility of shifting the zero dispersion wavelength of photonic crystal fibers and designing photonic crystal fibers with ultra-fla.
探讨了利用无量纲色散方法控制光子晶体光纤零色散点和设计平坦色散光子晶体光纤的可能性 。
2.
A Galerkin′s method based numerical procedure is used to design photonic crystal fibers with zero dispersion wavelength at 800 nm.
基于Galerkin方法计算并设计了在 80 0nm处具有零色散的光子晶体光纤。
2) the zero dispersion
零色散
1.
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 Schrodinger equatiton.
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。
3) near-zero dispersion
近零色散
4) zero dispersion point
零色散点
1.
It is indicated that the zero dispersion point is hardly influenced by the number of air holes in cladding with large relative apertures.
用多极方法数值研究构成六重对称全内反射型光子晶体光纤各种结构参数对基模零色散点的调节。
5) Zero dispersion region
零色散区
6) zero-dispersion wavelength
零色散波长
1.
It s a frequency-domain phase shift system designed to minimize systematic errors in measurements of zero-dispersion wavelength, and it has the λ0 characterized with an expanded uncertainty of 0.
主要介绍了一套高精度光纤色散测试系统,系统采用频域相移法测量光纤的零色散波长以减小系统误差的影响,其零色散波长测量不确定度达到了0。
2.
In this paper, the effects on the fiber optical parametric amplifier’s gain bandwidth which come from slope of the dispersion, zero-dispersion wavelength and birefringence are introduced.
光纤参量放大器在当今高速WDM光纤通信系统中有广泛的应用前景,宽带宽是其主要特性之一,本文在分析诸如光纤的色散平坦斜率、零色散波长及双折射因素对光纤参量放大器增益带宽的影响的基础上,论述了拓宽增益带宽的几种方法和设计技术。
3.
In the process of λ0 achieving and exceeding 820 nm which is the zero-dispersion wavelength of the fir.
在λ0达到并超过第一高阶模的零色散波长(820 nm)的过程中,抽运波工作在反常色散区,其向反斯托克斯波的能量转化逐渐增强。
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