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    • 11. 发明公开
    • OPTICAL MODULATOR
    • OPTISCHER调制器
    • EP2453295A1
    • 2012-05-16
    • EP10796926.3
    • 2010-07-09
    • Nippon Telegraph And Telephone Corporation
    • GOH, TakashiDOI, YoshiyukiMINO, ShinjiTSUZUKI, KenYAMAZAKI, HiroshiYAMADA, Takashi
    • G02F1/035G02B6/12G02B6/122
    • G02F1/0327G02B2006/12142G02B2006/12159G02F1/225G02F2201/126G02F2203/20G02F2203/21
    • In a nest MZI modulator in which each arm includes a child MZI, the power consumption in both of a relative phase adjusting section itself for adjusting the relative phase of an optical signal from a child MZI and the driving circuit of a relative phase adjusting section is reduced. The hybrid integrated-type nest MZI modulator of the embodiment 1a is configured so that, instead of placing a relative phase adjusting section in a parent MZI, a bias electrode Bias90° in which an electric field is applied in the same direction (or in an opposite direction) to the polarization direction in both of the upper and lower arms and a GND electrode are placed in each child MZI (see Fig. 4B ). The bias electrode Bias90° and the GND electrode provided in each child MZI constitute the entirety of a relative phase adjusting section. The optical signals are subjected to a phase change after the output from the child MZI (see Fig. 1A ), because such relative phase adjusting section can subject the optical signals of the upper and lower arms of the child MZI to a shift change in the same direction, respectively.
    • 在其中每个臂包括子MZI的嵌套MZI调制器中,用于调整来自子MZI的光信号的相对相位和相对相位调节部分的驱动电路的相对相位调整部分本身的功耗是 降低。 实施例1a的混合集成型嵌套MZI调制器被配置为使得不是将母相MZI中的相对相位调整部分放置在相同方向上施加电场的偏置电极Bias90° 相反方向)和上臂和下臂中的偏振方向,并且将GND电极放置在每个子MZI中(参见图4B)。 每个子MZI中设置的偏置电极Bias90°和GND电极构成相对相位调整部的整体。 光信号在从子MZI(参见图1A)的输出之后经历相变,因为这种相对相位调整部分可以使儿童MZI的上臂和下臂的光信号在 相同方向。
    • 12. 发明公开
    • THERMO-OPTICAL PHASE SHIFTER
    • 热电偶PHASENSCHIEBER
    • EP2136238A1
    • 2009-12-23
    • EP08712130.7
    • 2008-02-29
    • NEC Corporation
    • TAKAHASHI, MorioWATANABE, Shinya
    • G02F1/01G02B6/122G02B6/13
    • G02F1/011G02B2006/12142G02F1/0147G02F2203/15G02F2203/50
    • Provided is a thermo-optical phase shifter including a composite body having an optical waveguide formed by a core and a clad and having a ratio Δ of a difference between a core refractivity and a clad refractivity against the core refractivity which is 4% or above and a heater attached to the optical waveguide. The composite body has: a bridge structure portion arranged along a substrate surface and separate from the substrate surface via a void; and a fixed portion which supports the bridge structure portion with respect to the substrate and is continuous to the both ends of the bridge structure portion. The bridge structure has a half-circle-arc shape in the plane along the surface of the substrate.
    • 本发明提供一种热光学移相器,其包括具有由芯和包层形成的光波导的复合体,所述光波导的芯折射率和包层折射率与芯折射率的差为4%以上, 连接到光波导的加热器。 所述复合体具有:沿着基板表面布置并经由空隙与所述基板表面分离的桥结构部分; 以及固定部分,其相对于基板支撑桥结构部分,并且与桥结构部分的两端连续。 桥结构沿着衬底的表面在平面中具有半圆弧形状。
    • 18. 发明公开
    • Method for lattice matched growth of semiconductor layers
    • Verfahren zum gitterangepassten Aufwachsen von Halbleiterschichten
    • EP0689230A2
    • 1995-12-27
    • EP95304091.2
    • 1995-06-14
    • AT&T Corp.
    • Cunningham, John EdwardPathak, Rajiv NathGoossen, Keith Wayne
    • H01L21/20G02F1/015
    • G02F1/017B82Y20/00G02B2006/12142G02F2001/01766G02F2202/102G02F2203/02H01L21/02392H01L21/02461H01L21/02463H01L21/02507H01L21/02543H01L21/02546Y10S438/938
    • An in-situ method is disclosed for highly accurate lattice matching using reflection high energy electron diffraction dynamics. The method includes the steps of providing a substrate of a first semiconductor material and initiating growth of a second semiconductor material thereon. The oscillation amplitude of intensity I of waveform cycles is monitored using reflection high energy electron diffraction. A maximum intensity I + and a minimum intensity I - is determined over a predetermined number of waveform cycles. The intensity drop ΔI from initial reflectivity to minimum reflectivity of the waveform cycles is determined and a normalized figure of merit FM is calculated for the predetermined number of waveform cycles using the relationship: FM = Σ(I + - I - ) ΔI
      The fluxes of the second semiconductor material are then adjusted to maximize FM and optimize lattice matching.
      A multiple quantum well light modulator is also provided including a semiconductor substrate of InP, a multiple quantum well region, disposed above the InP substrate, composed of InGaAs and having a thickness of about 4 µm. The modulator is characterized by a lattice mismatch of less than 2 x 10 -4 .
    • 公开了一种使用反射高能电子衍射动力学进行高精度晶格匹配的现场方法。 该方法包括以下步骤:提供第一半导体材料的衬底并且在其上起始第二半导体材料的生长。 使用反射高能电子衍射监测波形周期的强度I的振荡幅度。 在预定数量的波形周期内确定最大强度I +和最小强度I 1。 确定从初始反射率到波形周期的最小反射率的强度降DELTA I,并且使用以下关系计算预定数量的波形周期的归一化品质因数FM:然后调整第二半导体材料的通量 以最大化FM并优化晶格匹配。 还提供了一种多量子阱光调制器,其包括设置在InP衬底上方的InGaAs并具有约4μm厚度的InP的多个量子阱区的半导体衬底。 调制器的特征在于小于2×10 -4的晶格失配。