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    • 4. 发明申请
    • High speed thermo-optic phase shifter and devices comprising same
    • 高速热电相移器及包括其的装置
    • US20040240818A1
    • 2004-12-02
    • US10448711
    • 2003-05-30
    • LUCENT TECHNOLOGIES INC.
    • Edward John LaskowskiChristi Kay MadsenAnnjoe Golangco Wong-Foy
    • G02B006/26G02B006/42G02B006/02G02B006/22
    • G02F1/011G02B6/138G02F1/0147G02F1/025G02F2001/0113
    • In accordance with the invention, a high speed thermo-optic phase shifter comprises a length of optical waveguide including a waveguiding core of a first material having an index of refraction n1 and a first order temperature dependence nulldn1/dTnull and, optically coupled to the core, a length of a second material having an index n2 preferably greater than the core (n2>n1) and a first order temperature dependence nulldn2/dTnull than the core (nulldn2/dTnull>nulldn1/dTnull). Advantageously, the length of second material is adiabatically tapered at both ends. Upon heating, as by a resistance heater, the second material changes the optical pathlength by an amount predominantly determined by nulldn2/dTnull providing faster switching speed. In a preferred embodiment, the core comprises silica, and the second material comprises silicon to produce switching speeds up to a few hundred MHz.
    • 根据本发明,高速热光移相器包括一段光波导,其包括具有折射率n1的第一材料的波导芯和一阶温度依赖性| dn1 / dT | 并且光学耦合到所述芯,具有指数n2的长度优选地大于所述芯(n2> n1)和第一阶温度依赖性| dn2 / dT | (| dn2 / dT |> | dn1 / dT |)。 有利地,第二材料的长度在两端是绝热的锥形。 在加热时,如电阻加热器那样,第二材料将光程长度改变主要由| dn2 / dT | 提供更快的切换速度。 在优选实施例中,芯包括二氧化硅,第二材料包括硅以产生高达几百MHz的切换速度。
    • 6. 发明申请
    • Optical transmission line
    • 光传输线
    • US20040165849A1
    • 2004-08-26
    • US10781719
    • 2004-02-20
    • THE FURUKAWA ELECTRIC CO., LTD.
    • Kazunori Mukasa
    • G02B006/22
    • G02B6/02009G02B6/02004G02B6/02252G02B6/02261G02B6/02266G02B6/02271G02B6/02276G02B6/0228G02B6/02285G02B6/0281G02B6/03611G02B6/03627G02B6/03633G02B6/03644G02B6/29377H04B10/25253
    • An optical transmission line according to the present invention is an optical transmission line which is able to control both the waveform distortion due to the non-linearity phenomenon and the waveform distortion due to dispersion. The optical transmission line is formed by connecting, in series, the first optical fiber (8), of which the dispersion value in the set wavelength band within the 1.5 nullm wavelength band is 6 to 14 ps/nm/km, and the second optical fiber (9), of which the dispersion value in said set wavelength band is null14 to null6 ps/nm/km. The dispersion slopes of the first optical fiber (8) and the second optical fiber (9) are of mutually opposite symbols. Light transmitted from an optical transmitter (11) enters the first optical fiber (8) and light which has been transmitted through the first optical fiber (8) enters the second optical fiber (9). The absolute value of the dispersion in the 1.5 nullm wavelength band of each of the optical fibers (8) and (9) is set to be 6 ps/nm/km or more so as to control the four light wave mixture and said absolute value is set to be 14 ps/nm/km or less so as to control a local dispersion, in order to set at approximately zero, for the entire optical transmission line, both the dispersion value and the dispersion slope in said set wavelength band.
    • 根据本发明的光传输线是能够控制由于非线性现象引起的波形失真和由于分散引起的波形失真的光传输线。 光传输线通过串联连接第一光纤(8),其中在1.5μm波长带内的设定波长带中的色散值为6至14ps / nm / km,第二光纤 光纤(9),其中所述设定波长带中的色散值为-14至-6ps / nm / km。 第一光纤(8)和第二光纤(9)的色散斜率相互相反。 从光发射器(11)发射的光进入第一光纤(8),并且已经透过第一光纤(8)的光进入第二光纤(9)。 将每个光纤(8)和(9)的1.5μm波长带中的色散的绝对值设定为6ps / nm / km或更大,以便控制四个光波混合和所述绝对值 设定为14ps / nm / km以下,以便对于整个光传输线,在所述设定的波长带中的色散值和色散斜率两者中控制局部色散以便设置为大约为零。
    • 10. 发明申请
    • Optical fibers and modules for dispersion compensation with simultaneous raman amplification
    • 用于色散补偿的光纤和模块,同时进行拉曼放大
    • US20040052486A1
    • 2004-03-18
    • US10243211
    • 2002-09-13
    • Fitel USA Corp.
    • Peter GaardeLars Gruner-NielsenChristian LarsenBera PalsdottirYujun Qian
    • G02B006/22
    • G02B6/03666G02B6/02261G02B6/03611G02B6/03644G02B6/29376H04B10/2525H04B10/2916
    • An optical fiber suited for dispersion compensation with simultaneous Raman amplification. The fiber has a central core and an index profile that defines successively concentric regions radially outward of the core. The core has a diameter of between 2 and 5 microns (nullm) and a refractive index difference (nulln) with respect to the outer cladding of between 0.012 and 0.035. A trench region adjacent the core is between 2 and 6 nullm wide and has a negative nulln of between null0.015 and null0.003. A ring region adjacent the trench region is between 1 and 5 nullm wide and has a nulln of between 0.001 and 0.015, and an inner cladding surrounding the ring region has a width of between zero and 5 nullm and a nulln of between null0.011 and 0.001. A dispersion slope compensating module (DSCM) including the fiber obtains a relatively high Raman gain with respect to conventional DSCMs that are pumped for Raman amplification.
    • 一种适用于同步拉曼放大的色散补偿的光纤。 纤维具有中心纤芯和折射率分布,该分布轮廓确定核心径向向外的连续同心区域。 芯的直径为2至5微米(mum),相对于外包层的折射率差(Deltan)为0.012至0.035。 与核心相邻的沟槽区域在2和6μm宽之间,并且具有-0.015和-0.003之间的负Deltan。 与沟槽区相邻的环形区域的宽度为1至5μm,并且具有介于0.001和0.015之间的Deltan,并且环形区域周围的内包层的宽度为零至5um之间,Deltan在-0.011和0.001之间 。 包括光纤的色散斜率补偿模块(DSCM)相对于泵浦拉曼放大的常规DSCM获得相对较高的拉曼增益。