首页>
外国专利>
Chirped fiber bragg grating - -, a laser system and method for the dispersive correction demands
Chirped fiber bragg grating - -, a laser system and method for the dispersive correction demands
展开▼
机译:fiber光纤布拉格光栅-色散校正要求的激光系统和方法
展开▼
页面导航
摘要
著录项
相似文献
摘要
Chirped fiber bragg grating - -,characterized in thatthe chirped fiber - bragg - grid (cfbgs) as a nonlinear chirped fiber - bragg - grid is formed, wherein the cfbgs within a predeterminable an angular frequency ω0 , and ω1 limited spectral range located at the bragg - wavelengths λB(l) are impressed in accordance with the following design rule:in which the penetration depth l (ω) described below, the equation with:l (ω): penetration depth into the cfbgs for light of wavelength λ = 2πc / ω,ω: angular frequency of the light,c: vacuum - speed of light,n (ω): refractive index of the fiber andGdds (ω): the groups running time dispersion, a first a freely selectable contribution c2 for the linear phase of the lattice structure of the cfbgs (zeroth order of the opening degree of dispersion, φ (ω)) and a further additional contribution c1 to the difference of the groups - and the phase delay of the cfbg (first order of dispersion, dφ (ω) / dω) coordinated in such a way that for the predetermined angular frequency ω1 a predetermined depth of penetration, preferably the maximum available length lges of the cfbg, is realized, and the impressed bragg - wavelengths λB(l), respectively, satisfy the following equation:where ω (l) the inverse..
展开▼
机译:rp光纤布拉格光栅-,其特征在于,形成了fiber光纤-布拉格-栅格(cfbgs)为非线性chi光纤-布拉格-栅格,其中,cfbg在预定的角频率ω 0 Sub>内,根据以下设计规则施加位于布拉格-波长λ B Sub>(l)的ω 1 Sub>有限光谱范围:其中穿透深度l(ω)如下所述,方程式为:l(ω):波长λ=2πc的光进入cfbgs的深度/ω,ω:光的角频率,c:真空-光速,n(ω):折射率和Gdds(ω)的乘积:组运行时间色散,是cfbgs晶格结构的线性相的第一自由选择贡献c 2 Sub>(色散开度的零阶, φ(ω))以及对组之差的进一步贡献c 1 Sub>-以及cfbg的相位延迟(色散的一阶,dφ(ω) /dω)以这样的方式进行协调:对于预定的角频率ω 1 Sub>,预定的穿透深度,最好是cfbg的最大可用长度l ges Sub>,所加的布拉格波长λ B Sub>(l)分别满足以下方程式:其中ω(l)逆。
展开▼