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    • 71. 发明授权
    • Holey waveguide manufacture
    • 多孔波导制造
    • US06738550B2
    • 2004-05-18
    • US10166724
    • 2002-06-12
    • Graham Town
    • Graham Town
    • G02B620
    • G02B6/105B29D11/00721C03B37/0122C03B2203/14C03B2203/42G02B6/02357G02B6/02361G02B6/0239
    • A method of forming a holey waveguide, the method comprising the steps of forming a guiding region of a preform, forming a cladding region of the preform, wherein at least a portion of the cladding region of the preform is formed from a plurality of cladding tubes of at least two different diameters, choosing at least one of the diameters of the cladding tubes in a manner such as to reduce a total number of cladding tubes required to build up said portion of the cladding region when compared with utilising cladding tubes of the same diameter for said portion, and drawing the waveguide from the preform.
    • 一种形成多孔波导的方法,所述方法包括以下步骤:形成预成型件的引导区域,形成预成型件的包层区域,其中预成型件的包层区域的至少一部分由多个包层管 至少两个不同的直径,以这样的方式选择包层管的直径中的至少一个,以便与使用相同的包层管相比,减少了建立包层区域的所述部分所需的包层管的总数 用于所述部分的直径,以及从预成型件拉制波导。
    • 73. 发明申请
    • Microstructuring optical wave guide devices with femtosecond optical pulses
    • US20040071420A1
    • 2004-04-15
    • US10632111
    • 2003-08-01
    • Omur M. SezermanKenneth O. HillGarland BestDwayne R. J. MillerMichael ArmstrongShujie Lin
    • G02B006/02G02B006/16
    • G02B6/02123C03C23/0025C03C25/6208G02B6/02052G02B6/02147G02B6/105G02B6/266G02B6/2821G02B6/2852G02B6/4214
    • The present invention is directed to the creation of zones of permanently altered refractive index characteristics in glass waveguiding devices, including optical fibers and optical waveguides pre-existed in a glass substrate. Such zones in which the refractive index has been permanently altered are created in glass using a very high intensity laser beam which is produced by focusing the light output from an ultrafast pulsed laser at a predetermined target region in the glass. The preferred laser is a Ti:Sapphire amplified, frequency-doubled Erbium-doped fiber laser system, providing light pulses of approximately 100 femtosecond duration, each with an energy of between about 1 nanojoule and 1 millijoule, and preferably at a pulse repetition rate of between 500 Hz and 1 GHz. The repetition rate is chosen to deliver pulses faster than the thermal diffusion time over the dimensions of the volume element being modified. This latter process is to accumulate heat to the point of liquefying the material in order to increase material compliance to the femtosecond writing process and increase the subsequent thermal barrier to relaxation of the written structural element and thereby increase the lifetime of the device or structural function. One or more zones of permanently altered refractive index characteristics can be formed in a waveguiding device, such as an optical fiber by utilizing a focused, pulsed, laser light source which generates a focal region having an intensity greater than the threshold for inducing permanent refractive index changes in the device. The focal region is aligned with the device and relative movement between the focal region and the device has the effect of sweeping the focal region across the device in a predetermined path. The result is a zone within the device in which the refractive index characteristics of the device have been permanently altered so as to control amplitude, phase, spatial propagation or polarization states of light within the material.
    • 74. 发明授权
    • All fiber polarization mode dispersion compensator
    • 全光纤偏振模色散补偿器
    • US06707977B2
    • 2004-03-16
    • US10056961
    • 2002-01-25
    • Ching-Kee ChienMichelle D FabianGregory F JacobsEdward F MurphyHuan-Hung ShengLung-Ming Wu
    • Ching-Kee ChienMichelle D FabianGregory F JacobsEdward F MurphyHuan-Hung ShengLung-Ming Wu
    • G02B627
    • G02B6/278C03C25/106G02B6/02395G02B6/105G02B6/274G02F1/0134
    • A polarization mode dispersion compensator corrects polarization mode dispersion in an optical signal having a fast polarization mode component, a slow polarization mode component and a time differential between the components. The compensator includes a phase shifter and a variable delay section. An input of the phase shifter is coupled to an optical device that provides an optical signal that exhibits polarization mode dispersion. The phase shifter functions to rotate the optical signal principal states of polarization to a desired orientation. The phase shifter engages a segment of an optical fiber that is coated with a radiation cured coatings. The coating composition is selected so that in response to a preload comprising the application of a stress of about 80 MPa to said coating at about 80° C. and after a stress-relaxation period of at least about 1 hour, at about 80° C., a residual stress exhibited by said coating comprises at least about 60 MPa, and the coating is capable of transmitting a transverse stress to the fiber to controllably change the birefringence of the fiber.
    • 偏振模色散补偿器校正具有快速偏振模式分量,慢偏振模分量和分量之间的时间差的光信号中的偏振模色散。 补偿器包括移相器和可变延迟部分。 移相器的输入耦合到提供呈现偏振模色散的光信号的光学装置。 移相器用于将光学信号的主要偏振状态旋转到期望的取向。 移相器接合涂覆有辐射固化涂层的光纤段。 选择涂料组合物,使得响应于预载荷,其包括在约80℃下施加约80MPa的应力到所述涂层,并且在至少约1小时的应力松弛时间后,在约80℃ 由所述涂层表现出的残余应力包括至少约60MPa,并且涂层能够向纤维传递横向应力以可控地改变纤维的双折射。
    • 79. 发明申请
    • POLARIZED WAVE SCRAMBLER AND OPTICAL SIGNAL TRANSMISSION APPARATUS
    • 极化波形扫描器和光信号传输装置
    • US20030185482A1
    • 2003-10-02
    • US10291498
    • 2002-11-12
    • Fujitsu Limited
    • Isao NAKAJIMA
    • G02B006/17
    • G02B6/2786G02B6/105G02B6/14G02B6/274
    • Abstract of DisclosureThe present invention provides a polarized wave scrambler and an optical signal transmission apparatus in which polarization mode dispersion, which causes degradation of a transmitted waveform, is suppressed, and which can be easily manufactured and are low-cost and stable. A polarized wave scrambler has a first polarization maintaining optical fiber and a second polarization maintaining optical fiber, wherein a constant component of a phase difference characteristic for optical frequency between a high-speed axis and a low-speed axis of the first polarization maintaining optical fiber is equal to that of the second polarization maintaining optical fiber, and a slope for optical frequency of the phase difference characteristic of the first polarization maintaining optical fiber is different from that of the second polarization maintaining optical fiber, wherein a plane of polarization of the linearly polarized optical signal is set to an angle between the high-speed axis and the low-speed axis of the first polarization maintaining optical fiber and the linearly polarized optical signal is supplied to the first polarization maintaining optical fiber, and wherein the first polarization maintaining optical fiber and the second polarization maintaining optical fiber are spliced such that the high-speed axis of the first polarization maintaining optical fiber corresponds to the low-speed axis of the second polarization maintaining optical fiber, and the low-speed axis of the first polarization maintaining optical fiber corresponds to the high-speed axis of the second polarization maintaining optical fiber.
    • 发明内容本发明提供一种极化波加扰器和光信号传输装置,其中抑制了发射波形劣化的偏振模色散,并且可以容易地制造并且成本低且稳定。 偏振波扰频器具有第一偏振维持光纤和第二偏振保持光纤,其中第一偏振维持光纤的高速轴和低速轴之间的光频率的相位差特性的恒定分量 与第二偏振维持光纤相同,并且第一偏振维持光纤的相位差特性的光频率的斜率与第二偏振保持光纤不同,其中线性偏振面 偏振光信号被设定为第一偏振保持光纤的高速轴和低速轴之间的角度,并且线偏振光信号被提供给第一偏振保持光纤,并且其中第一偏振保持光 光纤和第二极化保持光 纤维被拼接,使得第一偏振保持光纤的高速轴对应于第二保偏光纤的低速轴,并且第一偏振保持光纤的低速轴对应于高 - 第二偏振保持光纤的速度轴。
    • 80. 发明授权
    • GePSG core for a planar lightwave circuit
    • GePSG内核,用于平面光波电路
    • US06615615B2
    • 2003-09-09
    • US09895583
    • 2001-06-29
    • Fan ZhongJonathan G. Bornstein
    • Fan ZhongJonathan G. Bornstein
    • G02B610
    • G02B6/12023G02B6/105G02B6/122G02B6/132G02B2006/12169
    • A method of depositing a core layer for an optical waveguide structure of a planar lightwave circuit. A GePSG core for an optical waveguide structure of a planar lightwave circuit is fabricated such that the optical core comprises doped silica glass, wherein the dopant includes Ge and P. In depositing a core layer from which the optical core is formed, two separate doping gasses (e.g., GeH4 and PH3) are added during the PECVD process to make Ge and P doped silica glass (GePSG). The ratio of the Ge dopant and the P dopant is configured to maintain a constant refractive index within the core layer across an anneal temperature range and to reduce a formation of bubbles within the core layer. The ratio of the Ge dopant and the P dopant is also configured to reduce refractive index birefringence within the core layer across an anneal temperature range.
    • 一种沉积用于平面光波电路的光波导结构的芯层的方法。 制造用于平面光波电路的光波导结构的GePSG芯,使得光芯包括掺杂的石英玻璃,其中掺杂剂包括Ge和P.在沉积形成有光纤芯的芯层时,两个单独的掺杂气体 (例如,GeH 4和PH 3)在PECVD工艺中被添加以制造Ge和P掺杂的石英玻璃(GePSG)。 Ge掺杂剂和P掺杂剂的比例被配置为在整个退火温度范围内在芯层内保持恒定的折射率,并且减小芯层内的气泡的形成。 Ge掺杂剂和P掺杂剂的比例还被配置为在整个退火温度范围内降低芯层内的折射率双折射。