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    • 81. 发明申请
    • PLANAR LIGHTWAVE FOURIER-TRANSFORM SPECTROMETER
    • 平面光源FOURIER变换光谱仪
    • US20100245831A1
    • 2010-09-30
    • US12710765
    • 2010-02-23
    • Katsunari OKAMOTO
    • Katsunari OKAMOTO
    • G01J3/45H05K13/00
    • G01J3/4531G02F1/3136Y10T29/49002
    • A transform spectrometer implemented on a planar waveguide circuit (PLC), having an input optical signal waveguide carrying an input optical signal to be analyzed; a plurality of couplers, each connected to the input optical signal waveguide, and each including a coupler output for carrying a coupled optical signal related to the input optical signal. An array of interleaved, asymmetrical waveguide Mach-Zehnder interferometers (MZI) is formed on the PLC, each having at least one input MZI waveguide, each MZI input waveguide receiving a coupled optical signal from a respective coupler output; wherein at least some of the input MZI waveguides intersect in a common layer of the PLC, at an angle which allows their respective coupled optical signals to transmit without unacceptable attenuation. This arrangement improves spatial efficiency of the PLC, allowing more MZIs to be implemented, resulting in increased spectral resolution.
    • 实现在平面波导电路(PLC)上的变换光谱仪,具有承载要分析的输入光信号的输入光信号波导; 多个耦合器,每个耦合器连接到输入光信号波导,并且每个耦合器包括耦合器输出,用于承载与输入光信号相关的耦合光信号。 在PLC上形成交错的非对称波导马赫 - 曾德干涉仪(MZI)阵列,每个波导具有至少一个输入MZI波导,每个MZI输入波导从相应的耦合器输出接收耦合的光信号; 其中输入MZI波导中的至少一些波导在PLC的公共层中以允许它们各自的耦合的光信号传输而没有不可接受的衰减的角度相交。 这种布置提高了PLC的空间效率,允许实现更多的MZI,从而提高了光谱分辨率。
    • 82. 发明申请
    • LOW-LOSS LOW-CROSSTALK INTEGRATED DIGITAL OPTICAL SWITCH
    • 低损耗低成本数字光纤开关
    • US20100111470A1
    • 2010-05-06
    • US12265938
    • 2008-11-06
    • Solomon AssefaWilliam M. GreenYounghee KimJoris Van CampenhoutYurii Vlasov
    • Solomon AssefaWilliam M. GreenYounghee KimJoris Van CampenhoutYurii Vlasov
    • G02B6/26
    • G02F1/3136G02F1/2257G02F2001/0151G02F2001/311
    • An optical switch includes a plurality of optical interferometric structures is serially connected between at least one optical input node and two optical output nodes. A primary waveguide directly connects an optical input node and a first optical output node. A complementary waveguide, which is directly connected to a second optical output node, is evanescently coupled with the primary waveguide in a pair of optically coupled sections provided in each optical interferometric structure. Each optical interferometric structure also includes a pair of decoupled sections, which includes a primary decoupled section embedding a portion of the primary waveguide and a complementary decoupled section which includes a portion of the complementary waveguide. The complementary decoupled section is embedded in a phase tuning structure that allows modulation of the phase of the optical signal passing through. The optical switch provides less insertion loss, less crosstalk, and wider bandwidth than prior art optical switches.
    • 光开关包括多个光学干涉结构串联连接在至少一个光输入节点和两个光输出节点之间。 主波导直接连接光输入节点和第一光输出节点。 直接连接到第二光输出节点的互补波导与设置在每个光学干涉结构中的一对光耦合部分中的主波导ev逝地耦合。 每个光学干涉结构还包括一对解耦部分,其包括嵌入主波导的一部分的初级去耦部分和包括互补波导的一部分的互补去耦部分。 互补解耦部分被嵌入相位调谐结构中,允许调制通过的光信号的相位。 与现有技术的光开关相比,光开关提供较少的插入损耗,较少的串扰和更宽的带宽。
    • 83. 发明授权
    • Non-blocking switch having carbon nanostructures and Mach-Zehnder interferometer
    • 具有碳纳米结构和马赫 - 策德尔干涉仪的非阻塞开关
    • US07547907B2
    • 2009-06-16
    • US11026282
    • 2004-12-29
    • Dmitri E. Nikonov
    • Dmitri E. Nikonov
    • H01L29/06
    • G02F1/3136B82Y20/00G02F1/3137G02F2202/00G02F2202/36
    • In embodiments of the present invention, a non-blocking quantum interference switch includes a segmented electron wave coupler that splits an electron wave and couples its two parts to two arms of a Mach Zehnder interferometer. A voltage may be applied to an interferometer gate electrode to change the phase of the electron wave traveling in that arm. A second segmented electron wave coupler may receive the two electron waves from the interferometer arms and recombine them into one electron wave. If the two electron waves interfere constructively, then the recombined electron wave exits through one switch output port, which may be a “logical zero” switch port, and if the two electron waves interfere destructively, then the recombined electron wave exits through a second switch output port, which may be a “logical one” switch port.
    • 在本发明的实施例中,非阻塞量子干涉开关包括分割电子波耦合器,其分割电子波并将其两部分耦合到马赫曾德尔干涉仪的两个臂。 可以向干涉仪栅电极施加电压以改变在该臂中行进的电子波的相位。 第二分段电子波耦合器可以从干涉仪臂接收两个电子波并将它们复合成一个电子波。 如果两个电子波构成干涉,则复合电子波通过一个开关输出端口离开,该开关输出端口可以是“逻辑零”开关端口,如果两个电子电子波破坏性地干扰,则复合电子波通过第二开关 输出端口,可以是“逻辑1”交换机端口。
    • 89. 发明申请
    • OPTICAL DEVICE
    • 光学装置
    • US20080008412A1
    • 2008-01-10
    • US11856480
    • 2007-09-17
    • Masaharu DOI
    • Masaharu DOI
    • G02F1/035
    • G02F1/3136G02F1/225G02F2203/25
    • The present invention relates to an optical device including a branching unit for making branches of incident light in a first branch ratio, a phase adjusting unit for adjusting the relationship in phase among branched lights obtained by the branching unit and a combining/branching unit for combining the lights after the phase adjustment by the phase adjusting unit and for then making branches of the combined light in a second branch ratio, at least one of the first branch ratio and the second branch ratio being previously set at a branch ratio other than 1:1. This can realize an optical device capable of properly selecting output light with a different wavelength chirp quantity.
    • 本发明涉及一种光学装置,包括:分支单元,用于以第一分支比例进行入射光的分支;相位调整单元,用于调节由分支单元获得的分支光之间的相位关系;以及组合/分支单元,用于组合 通过相位调整单元进行相位调整之后的光,然后使第二分支比例的组合光分支,第一分支比和第二分支比中的至少一个预先设置为除了1: 1。 这可以实现能够适当地选择具有不同波长啁啾量的输出光的光学装置。
    • 90. 发明授权
    • Photonic crystal waveguide, homogeneous medium waveguide, and optical device
    • 光子晶体波导,均匀介质波导和光学器件
    • US07310468B2
    • 2007-12-18
    • US10565012
    • 2004-07-16
    • Shigeo KittakaKazuaki OyaKeiji Tsunetomo
    • Shigeo KittakaKazuaki OyaKeiji Tsunetomo
    • G02B6/10G02B6/12G02B6/26
    • G02F1/3136B82Y20/00G02B6/1225G02F2202/32
    • A photonic crystal waveguide and a homogeneous medium waveguide for enabling a steep bend and arrangement at an arbitrary angle with low propagation loss. A photonic crystal waveguide has a core formed by a photonic crystal having periodicity in the Y-direction. Electromagnetic wave is propagated by a band on the Brillouin zone boundary of the photonic band structure of the core. A side face of the core parallel to the Y-direction is in contact with a homogeneous medium having a refractive index of ns, and the condition of λ0/ns>aλ/(λ2/4+a2)0.5 is satisfied when the wavelength in vacuum of the electromagnetic wave is represented by λ0, the period of the photonic crystal is represented by a, and the period in the XZ-plane direction of the wave propagated through the core is represented by λ.
    • 一种光子晶体波导和均匀介质波导,用于以低传播损耗以任意角度进行陡峭的弯曲和布置。 光子晶体波导具有由在Y方向上具有周期性的光子晶体形成的核心。 电磁波由核心的光子带结构的布里渊区边界上的带传播。 平行于Y方向的芯的侧面与折射率为n 的折射率的均匀介质接触,并且λ<0 / 当真空中的波长为λ时,满足λλ/(λ2/4 + a 2) 电磁波由λ表示,光子晶体的周期由a表示,并且通过核传播的波的XZ平面方向上的周期由λ表示。