首页> 外国专利> Optical grating in optical lead mfr. esp. for dispersion compensator with waveguide gratings

Optical grating in optical lead mfr. esp. for dispersion compensator with waveguide gratings

机译:光学引线中的光栅mfr。尤其是用于带有波导光栅的色散补偿器

摘要

The method provides an optical grating (1) in an optical conductor or lead (2), which extends along a predetermined longitudinal axis (21) of the lead (2). The grating has, along this axis (21), a refractive index (n) at least approximating a periodically oscillating target waveform (11), and/or a grating amplitude (delta n) following a target waveform (13) and/or a grating constant (G) following a target waveform (15). The grating is produced by allowing a refractive index changing means to act on the lead material. At least one optical signal is sent along the axis (21) of the resulting grating (10). Using this signal, a complex optical spectrum of the grating is measured at least approximately. A pulse response of the grating is calculated at least approximately from the measured spectrum using an inverse Fourier transformation. The actual values of the refractive index and/or the grating amplitude and/or the grating constant are calculated from the calculated pulse response by solving a one-dimensional stray problem. A difference between the actual values and the target values is derived. These differences are balanced out, at least partly, by allowing a refractive index changing means e.g. irradiation, heat treatment, application of voltage etc., to act on the lead material.
机译:该方法在光导体或导线(2)中提供光栅(1),该光栅(1)沿着导线(2)的预定纵轴(21)延伸。光栅沿着该轴(21)具有至少近似于周期性振荡的目标波形(11)的折射率(n)和/或跟随目标波形(13)和/或a的光栅振幅(δn)跟随目标波形(15)的光栅常数(G)。通过允许折射率改变装置作用在引线材料上来产生光栅。沿着所得光栅(10)的轴(21)发送至少一个光信号。使用该信号,至少近似地测量光栅的复杂光谱。使用逆傅立叶变换至少近似地从所测量的光谱计算光栅的脉冲响应。通过解决一维杂散问题,从计算出的脉冲响应中计算出折射率和/或光栅幅度和/或光栅常数的实际值。得出实际值和目标值之间的差异。通过允许例如通过改变折射率的装置来至少部分地平衡这些差异。辐射,热处理,施加电压等,以作用于铅材料。

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