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    • 1. 发明授权
    • GeBPSG top clad for a planar lightwave circuit
    • GeBPSG顶部包层用于平面光波电路
    • US07160746B2
    • 2007-01-09
    • US09917438
    • 2001-07-27
    • Fan ZhongMichael Lennon
    • Fan ZhongMichael Lennon
    • H01L21/00C23C16/06
    • C23C16/401G02B6/122G02B2006/121
    • A method of depositing a top clad layer for an optical waveguide of a planar lightwave circuit. A GeBPSG top clad layer for an optical waveguide structure of a planar lightwave circuit is fabricated such that the top clad layer comprises doped silica glass, wherein the dopant includes Ge (Germanium), P (Phosphorus), and B (Boron). In depositing a top clad layer for the optical waveguide, three separate doping gasses (e.g., GeH4, PH3, and B2H6) are added during the PECVD (plasma enhanced chemical vapor deposition) process to make Ge, P and B doped silica glass (GeBPSG). The ratio of the Ge, P, and B dopants is configured to reduce the formation of crystallization areas within the top clad layer and maintain a constant refractive index within the top clad layer across an anneal temperature range. A thermal anneal process for the top clad layer can be a temperature within a range of 950C to 1050C. The GeBPSG top clad layer reduces the insertion loss of passive arrayed waveguide grating devices and active planar lightwave circuit devices.
    • 一种沉积用于平面光波电路的光波导的顶包层的方法。 制造用于平面光波电路的光波导结构的GeBPSG顶包层,使得顶包层包括掺杂的石英玻璃,其中掺杂剂包括Ge(锗),P(磷)和B(硼)。 在沉积用于光波导的顶部包覆层时,三个单独的掺杂气体(例如,GeH 4,PH 3 3和B 2 H) 在PECVD(等离子体增强化学气相沉积)工艺中添加制备Ge,P和B掺杂的石英玻璃(GeBPSG)的工艺。 Ge,P和B掺杂剂的比例被配置为减少顶部包层内的结晶区域的形成,并且在整个退火温度范围内在顶部包覆层内保持恒定的折射率。 用于顶部包层的热退火方法可以是在950℃至1050℃的范围内的温度。 GeBPSG顶层减少了无源阵列波导光栅器件和有源平面光波电路器件的插入损耗。
    • 3. 发明授权
    • Crack propagation stops for dicing of planar lightwave circuit devices
    • 裂纹传播停止用于平面光波电路器件的切割
    • US06895133B1
    • 2005-05-17
    • US09885627
    • 2001-06-20
    • Chris P. CalkinsRobert Cole
    • Chris P. CalkinsRobert Cole
    • G02B6/13G02B6/12
    • G02B6/13
    • One aspect of the present invention relates to a method of dicing a substrate containing a plurality of non-rectangular shaped optical integrated circuits, involving forming stop cracks in the wafer, each stop crack adjacent and substantially parallel one of the non-rectangular shaped optical integrated circuits, and cutting the substrate in a curvilinear manner substantially parallel to a stop crack. Another aspect of the present invention relates to an optical structure containing a substrate; a plurality of non-rectangular shaped optical integrated circuits on the substrate, each non-rectangular shaped optical integrated circuit having an active region; and at least one stop crack positioned adjacent each non-rectangular shaped optical integrated circuit.
    • 本发明的一个方面涉及一种切割含有多个非矩形形状的光学集成电路的衬底的方法,包括在晶片中形成停止裂纹,每个停止与非矩形形状的光学集成 电路,并以基本上平行于停止裂纹的曲线方式切割基板。 本发明的另一方面涉及一种含有基底的光学结构; 在所述基板上的多个非矩形的光集成电路,每个非矩形的光集成电路具有有源区; 以及邻近每个非矩形形状的光学集成电路定位的至少一个止动裂纹。
    • 4. 发明授权
    • Arrayed waveguide grating with waveguides of unequal widths
    • 具有不等宽度波导的阵列波导光栅
    • US06853769B2
    • 2005-02-08
    • US09870876
    • 2001-05-30
    • Kenneth McGreer
    • Kenneth McGreer
    • G02B6/10G02B6/34
    • G02B6/12011G02B6/105G02B6/12023
    • The present invention provides an arrayed waveguide such that each waveguide of the grating has a substantially uniform width, but the width of any single waveguide in the grating is selected based on a predetermined birefringence required for the waveguide. Generally, the narrowest grating waveguide has the longest overall length and the widest grating waveguide has the shortest overall length. The remaining intermediate waveguides have widths that are interpolated between the narrowest and widest waveguide gratings. With an appropriate width for each waveguide, an arrayed waveguide grating is provided that has low polarization dependent wavelength.
    • 本发明提供一种阵列波导,使得光栅的每个波导具有基本均匀的宽度,但是基于波导所需的预定的双折射来选择光栅中的任何单个波导的宽度。 通常,最窄的光栅波导具有最长的总长度,最宽的光栅波导具有最短的总长度。 剩余的中间波导具有在最窄和最宽波导光栅之间内插的宽度。 对于每个波导具有适当的宽度,提供具有低偏振相关波长的阵列波导光栅。
    • 5. 发明授权
    • Hybrid digital electro-optic switch
    • 混合数字电光开关
    • US5970186A
    • 1999-10-19
    • US816124
    • 1997-03-11
    • John T. KenneyRichard D. Sherman
    • John T. KenneyRichard D. Sherman
    • G02F1/313G02B6/26
    • G02F1/3132
    • A hybrid digital electro-optic switch has core and/or cladding areas that contain at least two different materials which undergo a change in their refractive index when an electric field is applied. One of the two different materials used in core regions, for example, has a change in refractive index that is less than the change in refractive index for the other material when the materials are exposed to the same electric field. A hybrid digital electro-optic switch functions by modulating the propagation constants of the eigenmodes of the switch with a voltage-induced refractive-index change, so that the propagation constants of the two materials are equal either in the presence or absence of the electric field. These electro-optic modulations change the evanescent coupling between the waveguides of the waveguide regions of the switch and transfer an optical signal that was input into one of the waveguides to a coupled waveguide. Compared to earlier digital electro-optic switch designs, the new switch has lower switching voltage, smaller device size, a sharper optical signal transfer, and wider manufacturing and use tolerances, and the switch can use a wide array of materials in its construction. The new switch can also be integrated with both the microstrip and coplanar traveling wave electrodes for very high speed photonic switching applications.
    • 混合数字电光开关具有包含至少两种不同材料的芯和/或包层区域,当施加电场时,它们的折射率发生变化。 例如,在芯区域中使用的两种不同材料中的一种,当材料暴露于相同的电场时,折射率的变化小于其它材料的折射率变化。 混合数字电光开关通过用电压引起的折射率变化来调制开关的本征模的传播常数来实现,使得两种材料的传播常数在存在或不存在电场时相等 。 这些电光调制改变了开关的波导区域的波导之间的消逝耦合,并将输入到波导中的一个的光信号传送到耦合波导。 与先前的数字电光开关设计相比,新开关具有较低的开关电压,更小的器件尺寸,更清晰的光信号传输,更宽的制造和使用公差,并且开关可以在其结构中使用各种各样的材料。 新开关也可以与微带线和共面行波电极集成,用于非常高速的光子开关应用。
    • 7. 发明申请
    • Method and apparatus for controlling waveguide birefringence by selection of a waveguide core width for a top cladding
    • 通过选择顶部包层的波导芯宽度来控制波导双折射的方法和装置
    • US20080240655A1
    • 2008-10-02
    • US12079930
    • 2008-03-28
    • Farnaz ParhamiLiang ZhaoFan Zhong
    • Farnaz ParhamiLiang ZhaoFan Zhong
    • G02B6/34G02B6/10
    • G02B6/12023G02B6/126
    • A method and apparatus for controlling waveguide birefringence by selection of a waveguide core width for a tuned top clad is described herein. In one example, a dopant concentration within a top cladding material is between 3-6% (wt.). Given a tuned top cladding composition, a width of the waveguide core is pre-selected such that birefringence is minimized, i.e., a zero, or near zero. The desirable width of the waveguide core is determined by calculating the distribution of stress in the top cladding over a change in temperature. From this distribution of stress, a relationship between the polarization dependent wavelength and variable widths of the waveguide in the arrayed waveguide grating are determined. This relationship determines a zero value, or near zero value, of polarization dependent wavelength for a given range of waveguide widths. Accordingly, the width of the waveguide may be selected such that the polarization dependent wavelength is minimized.
    • 本文描述了通过选择用于调谐顶部包层的波导芯宽度来控制波导双折射的方法和装置。 在一个实例中,顶部包层材料内的掺杂剂浓度在3-6%(重量)之间。 给定一个调整的顶部包层组成,预先选择波导芯的宽度,使得双折射最小化,即零或接近零。 通过计算在顶部包层中的应力在温度变化中的分布来确定波导芯的期望宽度。 根据这种应力分布,确定阵列波导光栅中波导的偏振相关波长与可变宽度之间的关系。 对于给定的波导宽度范围,该关系确定偏振相关波长的零值或近零值。 因此,可以选择波导的宽度使得偏振相关波长最小化。