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    • 42. 发明申请
    • OPTICAL FIBER LINK WITH PRIMARY AND COMPENSATING OPTICAL FIBERS
    • 光纤光纤连接与主要和补偿光纤
    • US20150086161A1
    • 2015-03-26
    • US14488558
    • 2014-09-17
    • CORNING INCORPORATED
    • Scott Robertson BickhamXin ChenMing-Jun LiDale Robert Powers
    • G02B6/42G02B6/028
    • G02B6/0288G02B6/02247G02B6/268
    • An optical fiber link that utilizes concatenated primary and compensating multimode optical fibers is disclosed. The primary optical fiber has a first relative refractive index profile with a first alpha value α40 of about 2.1 that provides for a minimum amount of intermodal dispersion of guided modes at a peak wavelength λP40 in the range from 840 nm to 860 nm, and has a first bandwidth BW40 of 2 GHz·km or greater. The compensating optical fiber has a second relative refractive index profile with a second alpha value α60, and wherein −0.9≦(α60−α40)≦−0.1, and a peak wavelength λP60 greater than 880 nm. The optical fiber link has improved bandwidth and data rates for first and second optical signals within first and second wavelength ranges, respectively.
    • 公开了一种利用连接的初级和补偿多模光纤的光纤链路。 主光纤具有第一相对折射率分布,其第一α值α40为约2.1,其提供在840nm至860nm范围内的峰值波长λP40处的导模的最小量的多式联运色散,并且具有 2GHz·km以上的第一带宽BW40。 补偿光纤具有第二相对折射率分布,其具有第二α值α60,并且其中-0.9≤n1E(α60-α40)< 1E-0.1,峰值波长λP60大于880nm。 光纤链路分别改善了在第一和第二波长范围内的第一和第二光信号的带宽和数据速率。
    • 43. 发明授权
    • Methods and apparatus for power-equalized optical frequency comb generation
    • 用于功率均衡的光学频率梳生成的方法和装置
    • US08447155B1
    • 2013-05-21
    • US13725869
    • 2012-12-21
    • Ram Photonics, LLC
    • Ping Piu KuoYauheni Myslivets
    • G02B6/00H04B10/04
    • G02B6/00G02B6/02247G02F1/353G02F1/383G02F1/39G02F2201/16G02F2203/26G02F2203/56
    • An optical device for generating a frequency comb includes an optical source and a first waveguide comprising a nonlinear optical medium operable to mix at least two input optical waves to generate a plurality of first optical waves. The optical device also includes a second waveguide concatenated to the first waveguide and characterized by a first dispersion characteristics and operable to compress the waveforms of the plurality of first optical waves and to reduce a frequency chirp introduced by the first waveguide. The optical device additionally includes a third waveguide concatenated to the second waveguide. The third waveguide comprises a nonlinear optical medium and is operable to mix the plurality of first optical waves to generate a plurality of second optical waves and to increase a total number of second optical waves with respect to a total number of first optical waves.
    • 用于产生频率梳的光学装置包括光源和包括可操作以混合至少两个输入光波以产生多个第一光波的非线性光学介质的第一波导。 光学装置还包括连接到第一波导的第二波导,其特征在于第一色散特性并且可操作以压缩多个第一光波的波形并且减少由第一波导引入的频率啁啾。 光学装置还包括连接到第二波导的第三波导。 第三波导包括非线性光学介质,并且可操作以混合多个第一光波以产生多个第二光波,并且相对于第一光波的总数增加第二光波的总数。
    • 44. 发明申请
    • Method of controlling longitudinal properties of optical fiber
    • 控制光纤纵向特性的方法
    • US20100148383A1
    • 2010-06-17
    • US12316740
    • 2008-12-15
    • David J. DiGiovanniJeffrey W. NicholsonPaul S. WestbrookMan F. Yan
    • David J. DiGiovanniJeffrey W. NicholsonPaul S. WestbrookMan F. Yan
    • B29D11/00G02B1/12
    • G02B6/02247C03C25/62
    • A method of creating optical fiber to exhibit predetermined length-dependent characteristics (e.g., chromatic dispersion, polarization mode dispersion, cutoff wavelength, birefringence) includes the steps of: characterizing the fiber's selected characteristic(s) as a function of length; and performing a “treatment” which modifies the refractive index over the given length to adjust the defined parameter to fall within a defined tolerance window. These steps may be repeated one or more times until the measure of the parameter falls with the defined tolerance limits. The treatment process may include, for example, a low energy actinic radiation exposure, anneal, mechanical strain, DC voltage, plasma application, etc. Indeed, if the treatment process is repeated, a different technique may be used to adjust the refractive index (“different” processes include, for example, modifying the strength/time of a UV exposure, temperatures for annealing, etc.).
    • 产生光纤以呈现预定长度相关特性(例如,色散,偏振模色散,截止波长,双折射)的方法包括以下步骤:将光纤的选定特性表征为长度的函数; 并且执行修改在给定长度上的折射率的“处理”,以将限定的参数调整到落入限定的公差窗内。 这些步骤可以重复一次或多次,直到参数的测量值与定义的公差极限一致。 处理过程可以包括例如低能量光化辐射暴露,退火,机械应变,DC电压,等离子体施加等。实际上,如果重复处理过程,则可以使用不同的技术来调节折射率( “不同”方法包括例如改变UV暴露的强度/时间,退火温度等)。
    • 48. 发明申请
    • Optical fiber and optical transmission path
    • 光纤和光传输路径
    • US20030215201A1
    • 2003-11-20
    • US10437052
    • 2003-05-14
    • FUJIKURA LTD.
    • Shoji TanigawaShoichiro MatsuoKuniharu HimenoKoichi Harada
    • G02B006/16G02B006/22
    • G02B6/03694G02B6/02247G02B6/02285G02B6/03611G02B6/03627G02B6/03644G02B6/03666G02B6/29377
    • Under condition that a non-circularity ratio is 5% or lower and a thermal expansion coefficient of a glass which forms the core is null1 and a thermal expansion of a glass which forms the cladding is null2, the difference of coefficients is controlled such that a formula null2.5null10null7/null C.nullnull1nullnull2null1.0null10null7/null C. is satisfied so as to maintain a polarization mode dispersion to be 0.03 ps/km0.5 or lower. The difference of coefficients is further controlled such that a formula null1.5null10null7/null C.nullnull1nullnull2null0/null C. is satisfied so as to maintain a polarization mode dispersion to be 0.015 ps/km0.5 or lower. By doing this, birefringence is reduced by adjusting the thermal expansion coefficient in a core and a cladding; thus providing an optical fiber, and an optical transmission path using the optical fiber, having preferable PMD for high speed transmission.
    • 在非圆度比为5%以下,形成芯的玻璃的热膨胀系数为α1,形成包层的玻璃的热膨胀为α2的条件下,控制系数差,使得 满足公式-2.5×10 -7 /℃。<=α1-α2<= 1.0×10 -7 /℃,以便将偏振模色散维持在0.03ps / km <0.5>或更低 。 进一步控制系数的差异,使得满足公式-1.5×10 -7 /℃<=α1-α2<= 0 /℃,以便将偏振模色散维持为0.015ps / km <0.5>以下。 通过这样做,通过调节芯和包层中的热膨胀系数来减少双折射; 从而提供一种光纤,以及使用该光纤的光传输路径,具有优选用于高速传输的PMD。
    • 50. 发明申请
    • Optical fiber, method of making the same, and optical transmission system including the same
    • 光纤,其制造方法以及包括该光纤的光传输系统
    • US20010046358A1
    • 2001-11-29
    • US09899020
    • 2001-07-06
    • SUMITOMO ELECTRIC INDUSTRIES, LTD.
    • Eisuke SasaokaMasashi OnishiKatsuya NagayamaKaoru OkunoKazuya Kuwahara
    • G02B006/16
    • G02B6/03644C03B37/0253C03B37/027C03B37/02745C03B37/032C03B2203/19C03B2203/36C03B2205/06G02B6/02247G02B6/02285G02B6/278
    • The present invention provides an optical fiber and the like comprising a structure making it possible to realize optical communications with a higher speed and a larger capacity as compared with conventional optical transmission systems. The optical fiber according to the present invention is an optical fiber in which at least one first portion having a positive chromatic dispersion at a predetermined wavelength within a wavelength band in use and at least one second portion having a negative chromatic dispersion at the predetermined wavelength are arranged adjacent each other along the longitudinal direction thereof. In particular, the optical fiber comprises a polarization coupling structure for inducing coupling between polarization modes of propagating light. This polarization coupling structure randomly causes coupling between polarization modes of the propagating light, whereby polarization mode dispersion decreases at the predetermined wavelength. As a consequence, transmission characteristics are effectively restrained from deteriorating due to polarization mode dispersion. Specifically, the polarization coupling structure is a twist applied to the optical fiber.
    • 本发明提供一种光纤等,其包括与常规光传输系统相比可以实现具有更高速度和更大容量的光通信的结构。 根据本发明的光纤是一种光纤,其中在使用中的波长带内的预定波长具有正色散的至少一个第一部分和在预定波长处具有负色散的至少一个第二部分是 沿着其纵向彼此相邻布置。 特别地,光纤包括用于在传播光的偏振模式之间引起耦合的偏振耦合结构。 该偏振耦合结构随机引起传播光的偏振模式之间的耦合,从而偏振模色散在预定波长处降低。 结果,由于偏振模式色散,传输特性被有效地抑制为劣化。 具体地,偏振耦合结构是施加到光纤上的扭转。