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    • 2. 发明申请
    • OPTICAL DISPERSION COMPENSATION
    • 光分散补偿
    • WO1998008121A1
    • 1998-02-26
    • PCT/GB1997002100
    • 1997-08-04
    • PIRELLI CAVI E SISTEMI S.P.A.LAMING, Richard, IanLOH, Wei-Hung
    • PIRELLI CAVI E SISTEMI S.P.A.
    • G02B06/16
    • G02B6/02109G02B6/02085G02B6/274G02B6/2746G02B6/278G02B6/29319G02B6/29394
    • A chirped optical fibre grating formed by impressing a chirped substantially periodic refractive index variation on a polarisation-maintaining optical fibre. The polarisation state of a laser transmitter (10) is maintained through an external modulator (20) and a polarisation maintaining circulator (30) by the use of polarisation maintaining fibre pigtails (40) aligned to one of the principal axes of high birefringence optical fibre used to fabricate the dispersion compensating grating (50). On reflection, light is output from the third port (60) of the circulator. Since only one polarisation mode of the grating (50) is excited, the PMD in the grating is eliminated. The polarisation maintaining circulator (30) comprises input/output lenses (32) at each port, a polarisation beam splitter (34) and a Faraday rotator (36). Light entering the circulator at the input port is arranged to be in a polarisation that passes through the polarisation beam splitter (34) towards the second port of the circulator. The light is rotated by 45 DEG in the rotator (36). The grating (50) and the fibre pigtail at the second port of the circulator are arranged with their principal axes rotated by 45 DEG with respect to the axes of the input to the circulator. Light reflected from the grating is then further rotated by 45 DEG by the rotator, into the polarisation which is deverted by the polarisation beam splitter (34). This light is therefore diverted to the third output (60) of the circulator. Another embodiment in which two chirped gratings (100, 110) are formed in high birefringence polarisation maintaining fibre with axes aligned, and a 45 DEG Faraday rotator (120) is placed inbetween.
    • 通过在偏振保持光纤上施加啁啾的基本上周期性的折射率变化而形成的啁啾光纤光栅。 激光发射器(10)的偏振状态通过使用与高双折射光纤的主轴之一对准的偏振保持光纤尾纤(40)通过外部调制器(20)和偏振保持环行器(30)来保持 用于制造色散补偿光栅(50)。 在反射时,从循环器的第三端口(60)输出光。 由于光栅(50)的仅一个偏振模式被激发,所以光栅中的PMD被消除。 偏振保持环行器(30)包括在每个端口处的输入/输出透镜(32),偏振分束器(34)和法拉第旋转器(36)。 在输入端口进入循环器的光被布置成处于朝向循环器的第二端口的偏振中。 灯在旋转器(36)中旋转45°。 循环器第二端口处的光栅(50)和光纤尾纤相对于循环器的输入轴旋转45°。 然后从光栅反射的光由旋转器进一步旋转45°,进入由偏振光束分离器(34)消除的偏振光。 因此,该光被转移到循环器的第三输出端(60)。 其中两个啁啾光栅(100,110)形成在具有轴对准的高双折射偏振保持光纤中的另一实施例,并且45°法拉第转子(120)放置在其间。