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    • 1. 发明授权
    • Non-blocking optical cross-connect structure for telecommunications
network
    • 用于电信网络的非阻塞光交叉连接结构
    • US5627925A
    • 1997-05-06
    • US418335
    • 1995-04-07
    • Rodney C. AlfernessAdel A. M. Saleh
    • Rodney C. AlfernessAdel A. M. Saleh
    • G02F1/313H04B10/02H04Q3/52H04Q11/00G02B6/28
    • H04Q11/0005H04Q2011/0009H04Q2011/0011H04Q2011/0015H04Q2011/0052
    • Wavelength division multiplexing, spatial switching cross-connect structures which may be deployed as intermediate nodes of an all optical network to route any input channel on any source fiber to any destination fiber at any available wavelength to achieve full connectivity between the nodes of the network. The non-blocking cross-connect structure comprises a wavelength division demultiplexer for receiving multiple wavelength channels from each source fiber and for separating received channels into N wavelengths so that the wavelengths are organized according to a corresponding fiber of origin, a nonblocking optical structure for spatially and independently rearranging the received wavelengths so that wavelengths having a common destination fiber are grouped together, and a wavelength division multiplexer for multiplexing together wavelengths having the same destination fiber.
    • 波分复用,空间交换交叉连接结构,其可以部署为全光网络的中间节点,以将任何源光纤上的任何输入信道路由到任何可用波长的任何目的地光纤,以实现网络节点之间的完全连接。 非阻塞交叉连接结构包括用于从每个源光纤接收多个波长信道并用于将接收信道分离为N个波长的波分解复用器,使得根据相应的原始光纤来组织波长,用于空间上的非阻塞光学结构 并且独立地重新布置所接收的波长,使得具有公共目的地光纤的波长被分组在一起;以及波分多路复用器,用于将具有相同目的地光纤的波长复用在一起。
    • 5. 发明授权
    • Polarization transformer
    • 极化变压器
    • US4384760A
    • 1983-05-24
    • US216309
    • 1980-12-15
    • Rodney C. Alferness
    • Rodney C. Alferness
    • G02B6/10G02B27/28G02F1/01G02F1/035G02F1/05H04B10/135G02B5/176
    • H04B10/25G02B6/105G02F1/0136G02F1/0353G02F2001/0142G02F2203/07
    • A generalized polarization transformer (10) is disclosed that is capable, under electrical control, of transforming the polarization of a signal between two arbitrary states. In its most general form, the transformer comprises a variable input phase shifter (11) for varying the relative phase between an incident pair of orthogonally polarized wave components; a variable mode converter (12) for varying the relative amplitudes of said orthogonally polarized wave components; and a variable output phase shifter (13) for varying the relative phase between the wave components derived from said mode converters. For some applications, the output phase shifter is not required. In an alternative configuration, the input phase shifter and the mode converter are combined in a common constructure.
    • 公开了一种能够在电气控制下将两个任意状态之间的信号的偏振变换的广义偏振变压器(10)。 在其最一般的形式中,变压器包括用于改变入射对的正交偏振波分量之间的相对相位的可变输入移相器(11) 用于改变所述正交极化波分量的相对振幅的可变模式转换器(12); 以及用于改变从所述模式转换器导出的波分量之间的相对相位的可变输出移相器(13)。 对于某些应用,不需要输出移相器。 在替代配置中,输入移相器和模式转换器组合在共同的结构中。
    • 6. 发明授权
    • Optical wavelength filter
    • 光波长滤波器
    • US4273411A
    • 1981-06-16
    • US114832
    • 1980-01-24
    • Rodney C. Alferness
    • Rodney C. Alferness
    • G02F1/035G02F1/313G02B5/14
    • G02F1/3132G02F1/0353G02F2201/066G02F2201/124G02F2203/055
    • An optical TE.revreaction.TM mode converter, using highly birefringent materials such as lithium niobate, is wavelength sensitive and, as such, can be used as a wavelength filter. However, to extract the filtered (i.e., the mode converted) signal, a separate, high quality polarization selective element is required. This application discloses means for eliminating the need for a separate polarization sensing element by using mode conversion as a means for spatially separating the filtered signal. The filter comprises a pair of mismatched waveguides (11, 12), and phase matching means (14, 15) for producing selective coupling between TE mode wave energy in one of the guides and TM mode wave energy on the other guide.
    • 使用诸如铌酸锂的高度双折射材料的光学TE - > TM模式转换器是波长敏感的,因此可以用作波长滤波器。 然而,为了提取滤波的(即,模式转换的)信号,需要单独的高质量偏振选择元件。 本申请公开了通过使用模式转换作为用于空间分离滤波信号的手段来消除对单独偏振感测元件的需要的装置。 滤波器包括一对失配的波导(11,12)和相位匹配装置(14,15),用于产生导向件之一中的TE模式波能量与另一个引导件上的TM模式波能量之间的选择性耦合。
    • 8. 发明授权
    • Asymmetric, periodically loaded waveguide for polarization rotation
    • 用于偏振旋转的不对称,周期性加载的波导
    • US5243669A
    • 1993-09-07
    • US864739
    • 1992-04-07
    • Rodney C. AlfernessThomas L. KochYosi Shani
    • Rodney C. AlfernessThomas L. KochYosi Shani
    • G02B6/12G02B6/126G02F1/01G02F1/025G02F1/035
    • G02F1/025G02B6/126G02F1/0353G02B2006/1204G02F2001/0142
    • Polarization rotation is achieved in an exemplary embodiment in an optical waveguide by augmenting the waveguide structure with a plurality of spaced-apart sections for loading the refractive index of the waveguide to cause a lateral asymmetry in the refractive index profile of the waveguide viewed in the plane transverse to the waveguide longitudinal axis. Each spaced-apart section induces non-zero coupling between the principal orthogonal polarization modes. Phase matched coupling between the principal orthogonal polarization modes is achieved by spacing the sections periodically by a distance .LAMBDA. equal to .lambda./.DELTA.N where .lambda. is the propagation wavelength in the waveguide and .DELTA.N is the difference between the effective refractive indices for the principal orthogonal polarization modes. Realizations of the waveguide structure are shown using Group III-V semiconductor rib waveguide structures.
    • 在光波导中的示例性实施例中通过用多个间隔开的部分来增加波导结构来实现极化旋转,以便加载波导的折射率以引起在平面中观察到的波导的折射率分布的横向不对称性 横向波导纵向轴线。 每个间隔开的部分在主正交偏振模式之间引起非零耦合。 主要正交偏振模式之间的相位匹配耦合是通过间隔这些部分周期性地等于λ/ DELTA N的距离LAMBDA来实现的,其中λ是波导中的传播波长,并且DELTA N是主正交的有效折射率之间的差 极化模式。 使用III-V族半导体肋波导结构示出了波导结构的实现。