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    • 1. 发明申请
    • OPTICAL PHASE REGENERATION METHOD AND DEVICE
    • 光相再生方法及器件
    • US20170078025A1
    • 2017-03-16
    • US15123122
    • 2015-02-09
    • NATIONAL INSTITUTE OF ADVANCED INDUSTRIAL SCIENCE AND TECHNOLOGY
    • Takayuki Kurosu
    • H04B10/299H01S5/50G02F1/35H04L7/00H04B10/556
    • H04B10/299G02F1/3536G02F1/3538G02F1/39G02F2001/354H01S5/06821H01S5/4006H01S5/50H01S5/5054H04B10/5561H04L7/0075
    • In a signal regeneration device in which recovery of a signal quality which has been degraded during transmission in optical communication and extension of a transmission distance are achieved, the most representative method of quantizing an optical phase is a phase sensitive amplifier (PSA) and a technique that utilizes an optical parametric process through use of a highly nonlinear optical medium, but there is a demand for a technique of quantizing an optical phase which is not accompanied with an optical parametric gain, has small-sized elements, is easily integrated, and does not require high power pump light. By a technique of a hybrid optical phase squeezer (HOPS), when a phase of input light is quantized to M levels (M>2), phase conjugate light of the input light and (M−1)th phase harmonic light of the input light are subjected to power modulation to be coherently added, so that quantization of the optical phase is performed through use of a simple four-wave mixing (FWM) that is not accompanied with the optical parametric gain and a general optical amplifier by using a general nonlinear optical medium such as silicon, and accordingly, a GER of equal to or higher than 30 dB can be obtained, even if a nonlinear optical element having a low nonlinearity is used.
    • 在实现在光通信中传输降低的信号质量的恢复和传输距离的扩展的信号再生装置中,量化光学相位的最具代表性的方法是相位敏感放大器(PSA)和技术 它通过使用高度非线性的光学介质利用光学参数化过程,但是需要量化光学相位的技术,其不伴随光学参数增益,具有小尺寸的元件,容易集成,并且 不需要大功率泵浦灯。 通过混合光学相位压缩器(HOPS)的技术,当输入光的相位被量化为M个电平(M> 2)时,输入光的相位共轭光和输入的第(M-1)相位相位谐波光 对光进行功率调制以进行相干相加,从而通过使用不伴随光参量增益的简单四波混频(FWM)和通用光放大器 非线性光学介质如硅,因此即使使用具有低非线性的非线性光学元件,也可以获得等于或高于30dB的GER。
    • 2. 发明授权
    • Conductively cooled liquid thermal nonlinearity cell for phase conjugation and method
    • 用于相位共轭的导电冷却液体热非线性电池及方法
    • US07589890B2
    • 2009-09-15
    • US11699848
    • 2007-01-30
    • Alexander A. BetinN. Peter DavisJoseph J. Ichkhan
    • Alexander A. BetinN. Peter DavisJoseph J. Ichkhan
    • H01S3/00G02B26/08
    • G02F1/3538G02F1/0147
    • A thermal nonlinear cell and method. The cell includes a substantially planar nonlinear medium and a mechanism for removing thermal energy from the medium in a direction substantially orthogonal to said medium. In one embodiment, the mechanism for removing thermal energy is a thermally conductive window mounted adjacent to the medium. Preferably, the mechanism includes plural thermally conductive windows between which the nonlinear medium is disposed. In the best mode, the windows are sapphire and the nonlinear medium is a fluid. The windows and the medium are transmissive with respect to first and second beams that interfere with each other and create an interference pattern in the cell. The interference pattern is sampled by a sampling hologram created within the multiple layers of the medium. The interference pattern is used via a sampling hologram to create a phase conjugate of a signal beam. The windows move thermal energy from the medium in a direction transverse to the longitudinal axis of the medium. This energy is then removed by heat sinks disposed at the ends of the stack of windows. In an alternative embodiment, the mechanism for removing thermal energy includes first and second mirrors mounted adjacent to the medium in a substantially parallel face-to-face relation. Preferably, the mirrors are heat exchangers such as slot-jet impingement coolers. In this embodiment, a transparent window is disposed between the mirrors and the nonlinear medium is disposed between the mirrors and the window. The mirrors are adapted to reflect first and second beams into the medium where they interfere to provide the interference pattern needed to create a phase conjugate beam.
    • 一种热非线性电池及方法。 电池包括基本平面的非线性介质和用于从基本上与所述介质正交的方向从介质去除热能的机构。 在一个实施例中,用于去除热能的机构是与介质相邻安装的导热窗。 优选地,该机构包括多个导热窗口,非线性介质之间设置有多个导热窗口。 在最佳模式下,窗户是蓝宝石,非线性介质是流体。 窗口和介质相对于彼此干扰并在单元中产生干涉图案的第一和第二波束是透射的。 通过在介质的多层内产生的采样全息图对干涉图案进行采样。 通过采样全息图使用干涉图案以产生信号光束的相位共轭。 这些窗口从介质沿与介质的纵轴垂直的方向移动热能。 然后通过设置在窗户堆叠的端部处的散热器去除该能量。 在替代实施例中,用于去除热能的机构包括以基本平行的面对面关系安装在介质附近的第一和第二反射镜。 优选地,反射镜是热交换器,例如喷射式冲击冷却器。 在本实施例中,透明窗设置在反射镜之间,并且非线性介质设置在反射镜和窗口之间。 这些反射镜适于将第一和第二光束反射到介质中,在那里它们干涉以提供产生相位共轭光束所需的干涉图案。
    • 3. 发明申请
    • Stimulated brillouin scattering phase conjugate mirror utilizing photonic bandgap guide and method
    • 利用光子带隙引导和方法的刺激布里渊散射相位共轭反射镜
    • US20050185907A1
    • 2005-08-25
    • US10786342
    • 2004-02-25
    • Robert ByrenDavid RockwellAlexander Betin
    • Robert ByrenDavid RockwellAlexander Betin
    • G02B6/02G02F1/35H01S3/10H01S5/14G02B6/20
    • G02F1/3538G02B6/02347G02B6/02385G02F2202/32H01S3/10076H01S5/145
    • A phase conjugate mirror comprising a photonic band gap light guide and a stimulated Brillouin scattering medium disposed in operational relation thereto. In specific embodiments, the light guide is an optical fiber with a high index cladding transparent at a propagation wavelength and a hollow or solid core. The cladding is microstructured silica and supports guide modes through frustrated tunneling photonic band gap guidance or Bragg photonic band gap guidance. The fiber has an array of channels disposed around the core. In one embodiment, the fiber is disposed within a stimulated Brillouin scattering cell. In this embodiment, the medium is gas, gel, or liquid. In an alternative embodiment, the medium is a solid disposed at the core of the fiber. The invention provides a means of guiding light with a gas filled or solid core structure with high guiding efficiency, high reflection back into the medium, without disturbing the polarization state of the light as it propagates.
    • 一种相位共轭反射镜,包括光子带隙光导和被布置在其中的布里渊散射介质。 在具体实施例中,光导是具有在传播波长处透明的高折射率包层和中空或实芯的光纤。 包层是微结构二氧化硅,通过挫折隧道光子带隙引导或布拉格光子带隙引导支持引导模式。 纤维具有围绕芯部设置的通道阵列。 在一个实施例中,光纤设置在受激布里渊散射单元内。 在该实施例中,介质是气体,凝胶或液体。 在替代实施例中,介质是设置在纤维芯部的固体。 本发明提供了一种将具有高引导效率的气体填充或实心芯结构引导光的方法,并将高反射回到介质中,而不会在光线传播时干扰光的偏振状态。
    • 4. 发明申请
    • Tunable optical signal oscillator
    • 可调光信号振荡器
    • US20020146046A1
    • 2002-10-10
    • US10106201
    • 2002-03-27
    • Samsung Electronics Co., Ltd.
    • A-jung KimYoung-kwang Seo
    • H01S003/10
    • H01S5/4006G02F1/3538H01S5/06213H01S5/0623
    • A tunable optical oscillator that generates optical signals at a band of micro- to millimeter-wave is provided. The tunable optical oscillator includes an electrical signal generator for generating an electrical signal at the predetermined band; a master laser that is driven by the electrical signal, and generates an optical signal having a first frequency; and a slave laser that is driven by an electrical signal, injected into the optical signal generated by the master laser, generates an optical signal having a second frequency, and mixes the received optical signal with the optical signal having a second frequency to be output. The tunable optical oscillator is capable of generating signals over a broadband including micro- to millimeter-wave and beyond, say, from tens of MHz to several THz. The generated signals by the optical oscillator have also frequency tunability over the range of tens of GHz with coarse tuning methods to tens of MHz with fine tuning methods.
    • 提供了一种在微毫米波段产生光信号的可调光学振荡器。 可调谐光学振荡器包括用于产生预定频带的电信号的电信号发生器; 由所述电信号驱动的主激光器,并产生具有第一频率的光信号; 以及被注入到由主激光器产生的光信号中的由电信号驱动的从属激光器,产生具有第二频率的光信号,并将接收到的光信号与具有要输出的第二频率的光信号进行混合。 可调谐光学振荡器能够通过包括微米到毫米波在内的宽带产生信号,例如从几十MHz到几个THz。 光学振荡器产生的信号在数十GHz的范围内也具有频率可调谐性,通过微调方法可以用微调方法将其调谐到数十MHz,并具有微调方法。
    • 9. 发明授权
    • Apparatus and method for steering a phase conjugate wave
    • 用于转向相位共轭波的装置和方法
    • US5093834A
    • 1992-03-03
    • US688650
    • 1991-04-19
    • David J. Morris
    • David J. Morris
    • G02F1/35
    • G02F1/3538
    • Four-wave mixing is used to produce a steered optical phase conjugate wave. First and second pump waves are combined with a probe wave in a nonlinear medium within an optical conjugate, producing an optical phase conjugate wave. The magnitude of the wave vectors corresponding to the first and second pump waves are different, causing the optical phase conjugate wave to define a non-zero angle .theta..sub.0 relative to the probe wave. In a first embodiment, the wavelengths of the first and second pump waves are controlled to vary the angle, while in a second embodiment, the intensities of the two pump waves are modified.
    • 四波混频用于产生转向光相位共轭波。 第一和第二泵浦波与光共轭中的非线性介质中的探测波组合,产生光相位共轭波。 对应于第一和第二泵浦波的波矢量的大小是不同的,使光相位共轭波相对于探测波定义非零角度θ0。 在第一实施例中,控制第一和第二泵浦波的波长以改变角度,而在第二实施例中,两个泵浦波的强度被改变。