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    • 31. 发明授权
    • MZM linear driver for silicon photonics
    • 用于硅光子学的MZM线性驱动器
    • US09454059B1
    • 2016-09-27
    • US14472193
    • 2014-08-28
    • INPHI CORPORATION
    • Radhakrishnan L. Nagarajan
    • G02F1/225G02F1/025G02F1/21G02F1/015
    • G02F1/0121G02F1/0123G02F1/025G02F1/225G02F1/2255G02F1/2257G02F2001/0154G02F2001/212H04B10/25H04B10/505H04L7/0075
    • The present invention includes a linear driver for Mach-Zehnder modulator (MZM) configured in a differential form with two waveguides carrying two traveling waves. Each waveguide comprises a MZM material configured with either a single segment in 3×MZM length or two split segments with one in 2×MZM length and another one in either 1× or 2×MZM length. By coupling a DC current source supplied with a modulation voltage with each segment thereof for providing electrical modulation signal overlapping with each of the two traveling waves. The modulated traveling waves in the two waveguides then are combined in one output signal by a multimode interference coupler. By properly choosing the configuration of MZM linear segments with optional length ratios, a low power consumption MZM linear driver provides either NRZ or PAM-4 modulation scheme to the input optical signals for telecommunication through silicon photonics.
    • 本发明包括一种以差分形式配置的马赫曾德尔调制器(MZM)的线性驱动器,其具有两个携带两个行波的波导。 每个波导包括配置有3×MZM长度的单个段或具有2×MZM长度的2个分割段的MZM材料,以及1×或2×MZM长度的另一个。 通过将提供有调制电压的DC电流源与其每个段耦合以提供与两个行波中的每一个重叠的电调制信号。 然后,两个波导中的调制行波由多模干涉耦合器组合在一个输出信号中。 通过适当选择具有可选长度比的MZM线性段的配置,低功耗MZM线性驱动器为通过硅光子学的电信输入光信号提供NRZ或PAM-4调制方案。
    • 35. 发明申请
    • SEMICONDUCTOR OPTICAL MODULATOR
    • 半导体光学调制器
    • US20100142026A1
    • 2010-06-10
    • US12530569
    • 2008-02-06
    • Tomoaki Kato
    • Tomoaki Kato
    • G02F1/03
    • G02F1/025G02F2001/0154G02F2201/127
    • An optical modulator is provided with a stripe-shaped optical waveguide, which has an upper clad layer, a lower clad layer formed between the upper clad layer and a substrate, and an undoped core layer which is arranged between the upper clad layer and the lower clad layer and has a complex refractive index that changes corresponding to the intensity of an applied electric field, to a signal light propagating inside. On the both sides of the stripe-shaped optical waveguide, conductor walls are configured by arranging a pair of parallel blocking flat boards with an insulating wall in between. Thus, the semiconductor optical modulator having a high optical modulation efficiency is provided
    • 光调制器设置有条形光波导,其具有上覆盖层,形成在上覆盖层和基板之间的下覆盖层,以及布置在上覆层和下层之间的未掺杂芯层 并且具有与施加的电场强度相对应的复合折射率与内部传播的信号光。 在条形光波导的两侧,导体壁通过在其间布置一对具有绝缘壁的平行阻挡平板而构成。 因此,提供了具有高光调制效率的半导体光调制器
    • 37. 发明授权
    • Electro-optic waveguide device
    • 电光波导器件
    • US5239598A
    • 1993-08-24
    • US746343
    • 1991-08-16
    • David R. WightJohn M HeatonMeirion F. LewisChristopher L. West
    • David R. WightJohn M HeatonMeirion F. LewisChristopher L. West
    • G02F1/015G02F1/025G02F1/295
    • G02F1/025G02F1/295G02F2001/0154
    • An electro-optic waveguide device (10) comprises an assembly of waveguides (30) connected to a common light input region (41) and forming a common far field diffraction pattern (44). The device (10) comprises an n.sup.+ GaAs substrate (14) bearing a waveguide lower cladding layer (16) of n.sup.+ Ga.sub.0.9 Al.sub.0.1 As, which is in turn surmounted by a waveguide core layer (18) of n.sup.- GaAs. The layer (18) has grooves (20) defining the waveguides (30), each of which has a respective Schottky contact (32). Each contact (32) is biased negative with respect to the substrate (14), which reverse biases the respective Schottky diode waveguide structure. The waveguide core layer (18) has electro-optic properties, and its refractive index varies with electric field. The phase of light emerging from each waveguide is therefore independently variable by means of its applied bias voltage. The waveguides (30) are arranged to provide output confined very largely to lowest order spatial modes, so that they produce a single far field diffraction pattern (44). Varying the set of bias voltages applied to the waveguides (30) produces output phase variation which changes the position of the diffraction pattern principal maximum (46) to produce beam steering.
    • 电光波导装置(10)包括连接到公共光输入区域(41)并形成公共远场衍射图案(44)的波导组件(30)。 装置(10)包括带有n + Ga0.9Al0.1As的波导下包层(16)的n + GaAs衬底(14),其又由n-GaAs的波导芯层(18)覆盖。 层(18)具有限定波导(30)的凹槽(20),每个波导具有相应的肖特基接触(32)。 每个触点(32)相对于衬底(14)偏置为负,这反向偏置相应的肖特基二极管波导结构。 波导芯层(18)具有电光性质,其折射率随电场而变化。 因此,从每个波导出射的光的相位可以通过其施加的偏置电压独立地变化。 波导(30)被布置成提供非常大地限制在最低阶空间模式的输出,使得它们产生单个远场衍射图案(44)。 改变施加到波导(30)的偏置电压的集合产生输出相位变化,其改变衍射图案主要最大值(46)的位置以产生波束转向。