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    • 1. 发明公开
    • OPTICAL INTERFERENCE FILTER DEVICE, ESPECIALLY FOR AN OPTICAL WAVELENGTH LOCKING DEVICE
    • 光学干涉滤光器装置,特别是用于光学波长锁定装置
    • EP3321720A1
    • 2018-05-16
    • EP16198701.1
    • 2016-11-14
    • ADVA Optical Networking SE
    • Wohlfeil, Benjamin
    • G02B6/293H01S5/068H04B10/50
    • G02B6/29338G02B6/29343G02B6/29344G02B6/29347G02B6/29389G02B6/4215H01S3/08027H01S5/026H01S5/0261H01S5/0687H01S5/141H04B10/5057H04B10/572
    • The invention relates to an optical interference filter device (126), especially for an optical wavelength locking device (110), which defines a first periodic filter frequency response between a first filter output port (130) and a filter input port (128) and a second periodic filter frequency response having the same free spectral range (FSR M ) as the first periodic frequency response between a second filter output port (132) and the filter input port (128), wherein the first and second periodic filter frequency responses are shifted versus each other by a predetermined optical frequency distance (fsr 12 ). According to the invention the optical interference filter device (126) comprises an optical ring resonator structure (152) and an optical combining and phase shifting structure (154). The optical ring resonator structure (152) comprises two optically coupled ring-shaped optical waveguides (160, 162), each of which is further coupled to a dedicated optical port waveguide (156, 158), wherein one (156) of the optical port waveguides (156, 158) defines the filter input port (128) at a first end thereof and first resonator output port (164) at a second end thereof and wherein the other (158) of the optical port waveguides (156, 158) has an open first end (166) and defines a second resonator output port /168) at a second end thereof. The optical combining and phase shifting structure (154) has a first and second input port (178, 182) and a first and second output port, the first input port (178) being connected to the first resonator output port (164) and the second input port (182) being connected to the second resonator output port (168), the first and second output ports defining the first and second filter output ports (130, 132), respectively. The optical combining and phase shifting structure (154) further comprises a first crossover path (190) between the first input port (178) and the second output port, a second crossover path 192) between the second input port (182) and the first output port, a first pass-through path (194) between the first input port (178) and the first output port and a second pass-through path (196) between the second input port (182) and the second output port, wherein in both pass-through paths (194, 196) and/or both crossover paths (190, 192) optical phase shifting means (198, 200; 198', 200') are provided which are configured to effect a phase shift difference of plus or minus 90 degrees between the optical signals that are guided in the first pass-through path (194) and the second crossover path (192) and a phase shift difference of minus or plus 90 degrees between the optical signals that are guided in the second pass-through path (196) and the first crossover path (190).
    • 本发明涉及一种特别用于光波长锁定装置(110)的光学干涉滤波器装置(126),其在第一滤波器输出端口(130)和滤波器输入端口(128)之间限定第一周期性滤波器频率响应,以及 具有与第二滤波器输出端口(132)和滤波器输入端口(128)之间的第一周期性频率响应相同的自由频谱范围(FSRM)的第二周期性滤波器频率响应,其中第一和第二周期性滤波器频率响应被移位 相互之间相隔预定的光学频率距离(fsr12)。 根据本发明,光学干涉滤波器装置(126)包括光学环形谐振器结构(152)和光学组合和相移结构(154)。 光学环形谐振器结构(152)包括两个光学耦合的环形光学波导(160,162),每个光学耦合环形光学波导进一步耦合到专用光学端口波导(156,158),其中光学端口 波导(156,158)在其第一端限定了滤波器输入端口(128)并且在其第二端限定了第一谐振器输出端口(164),并且其中光学端口波导(156,158)的另一个(158)具有 开放的第一端(166)并且在其第二端处限定第二谐振器输出端口/ 168)。 光学组合和相移结构(154)具有第一和第二输入端口(178,182)以及第一和第二输出端口,第一输入端口(178)连接到第一谐振器输出端口(164),并且第一 第二输入端口(182)连接到第二谐振器输出端口(168),第一和第二输出端口分别限定第一和第二滤波器输出端口(130,132)。 光学组合和相移结构(154)还包括第一输入端口(178)和第二输出端口之间的第一交叉路径(190),第二输入端口(182)和第一输入端口 输出端口,第一输入端口(178)和第一输出端口之间的第一直通路径(194)以及第二输入端口(182)和第二输出端口之间的第二直通路径(196),其中 在两个通过路径(194,196)和/或两个交叉路径(190,192)中,提供光学相移装置(198,200; 198',200'),其被配置为实现正相移 或第一交叉路径(192)中引导的光学信号与第二交叉路径(192)中引导的光学信号之间的相移差为负或正90度 直通路径(196)和第一交叉路径(190)。
    • 5. 发明公开
    • Optical fiber terminations, optical couplers and optical coupling methods
    • EndstückefürLichtleitfasern,optische Koppler und optische Kopplungsverfahren
    • EP1245973A1
    • 2002-10-02
    • EP01303031.7
    • 2001-03-30
    • UNIVERSITY OF SOUTHAMPTON
    • Grudinin, Anatoly BorisovichNilsson, JohanClarkson, William Andrew
    • G02B6/26H01S3/094
    • G02B6/29347G02B6/262G02B6/29317G02B6/29394G02B6/32H01S3/0672H01S3/06729H01S3/094003H01S3/094007H01S3/094019
    • An optical coupler for coupling a signal light beam from a signal port (100) and a pump light beam from a pump port (110) into a common port (120) for coupling the pump and signal beams into a double-clad (DC) optical fiber (122) comprising a core (123), an inner clad (124) and an outer clad (125). The DC optical fiber has a section of coreless fiber (128) joined to it to form an extension piece. A free-space optical arrangement (130) combines the pump and signal light beams onto the common port so that the signal light beam is focused onto the core aperture at the buried interface (121) between the DC optical fiber and the coreless extension piece. The high power density signal beam focus is thus moved away from a more sensitive air:glass interface into a buried interface which has a higher damage threshold. In this way, higher signal beam powers can be handled. The invention allows higher power DC pumped amplifiers and lasers to be fabricated.
    • 一种光耦合器,用于将来自信号端口(100)的信号光束和来自泵端口(110)的泵浦光束耦合到公共端口(120)中,用于将泵浦信号光束和信号光束耦合到双包层(DC) 包括芯(123),内包层(124)和外包层(125)的光纤(122)。 DC光纤具有连接到其上的无芯纤维(128)部分以形成延伸件。 自由空间光学装置(130)将泵浦信号光束和信号光束组合到公共端口上,使得信号光束聚焦在DC光纤和无芯延伸片之间的掩埋接口(121)处的芯孔上。 因此,高功率密度信号光束聚焦从更敏感的空气:玻璃界面移动到具有较高损伤阈值的掩埋界面中。 以这种方式,可以处理更高的信号光束功率。 本发明允许制造更高功率的直流泵浦放大器和激光器。
    • 6. 发明公开
    • Low dispersion interleaver
    • Verschachteler mit geringer色散
    • EP1235086A2
    • 2002-08-28
    • EP02251219.8
    • 2002-02-22
    • JDS Uniphase Inc.JDS Uniphase Corporation
    • Copner, NigelTan, Kim LeongAbraham, Christopher JohnDucellier, ThomasPicard, Marie Josee
    • G02B6/293
    • G02B6/12007G02B6/272G02B6/2766G02B6/2773G02B6/29302G02B6/29347G02B6/29349G02B6/29352G02B6/29358G02B6/29386
    • The present invention relates to an interferometer useful in the interleaving and deinterleaving of optical wavelength channels. Typically the invention comprises a beamsplitter and two resonators, e.g. GT etalons or ring resonators. The beamsplitter splits an input beam of light into a first sub-beam directed to follow a first path and a second sub-beam directed to follow a second path. The first resonator has a first effective cavity length and receives the first sub-beam. The second resonator has a second effective cavity length and receives the second sub-beam. The first path and the second path have an effective optical path difference approximately equal to one-half the first effective cavity length. In one embodiment, the front plates of the GT etalons each have a different reflectivity, and are selected to provide a desired spectral response. In another embodiment, the two resonators are slightly de-phased from one another such that the positive dispersion slope of the first resonator is aligned with the negative dispersion slope of the second resonator. Polarization-based versions of the invention are disclosed, in which a single resonator receives both sub-beams, which are orthogonally polarized. Single etalon versions of the invention are also possible, in which a beam is separated into sub-beams (i.e. reflected and transmitted beams) within a non-linear interferometer, and then re-combined outside the interferometer with the appropriate effective optical path length delay therebetween.
    • 本发明涉及可用于光波长信道的交织和解交织的干涉仪。 通常,本发明包括分束器和两个谐振器,例如。 GT标准具或环形谐振器。 分束器将输入光束分成指向跟随第一路径的第一子光束和指向跟随第二路径的第二子光束。 第一谐振器具有第一有效腔长并接收第一子光束。 第二谐振器具有第二有效腔长度并且接收第二子光束。 第一路径和第二路径具有大致等于第一有效腔长度的一半的有效光程差。 在一个实施例中,GT标准具的前板各自具有不同的反射率,并且被选择以提供期望的光谱响应。 在另一个实施例中,两个谐振器彼此稍微去相位,使得第一谐振器的正色散斜率与第二谐振器的负色散斜率对准。 公开了本发明的基于偏振的版本,其中单个谐振器接收正交极化的两个子光束。 本发明的单个标准具版本也是可能的,其中将光束分离成非线性干涉仪内的子光束(即反射和透射光束),然后在干涉仪外部以适当的有效光程长度延迟重新组合 其间。
    • 9. 发明公开
    • Integrated photonic devices with reduced sensitivity to external influences
    • 与外部影响的敏感性降低集成光子器件
    • EP2741113A1
    • 2014-06-11
    • EP13196054.4
    • 2013-12-06
    • IMECUniversiteit Gent
    • Dwivedi, SarvagyaBogaerts, Wim
    • G02B6/293G02B6/12
    • G02F1/011G02B6/12007G02B6/1225G02B6/125G02B6/29347G02B6/29398G02F2001/212G02F2203/15G02F2203/21G02F2203/60
    • Photonic device (100) having a wavelength-dependent transmission or filter characteristic, comprising: a Splitter Polarization Rotator (11) receiving polarized light (1) and providing a first resp. second wave (2, 3); a first resp. second waveguide arm (12, 13) connected to the SPR for propagating a first resp. second polarization mode (TM, TE) of the first resp. second wave (2, 3), the second polarization mode (TE) being different from the first polarization mode (TM); and a Polarization Rotator and Combiner (14) for combining the propagated first resp. second waves (2, 3); wherein the dimensions of the first and second arm (12, 13) are selected to cancel the influence of an external effect on the wavelength-dependent characteristic.
      Method for reducing the sensitivity of said integrated photonic device, comprising splitting a polarized light beam (1), and propagating light waves(2,3) of different polarity through two waveguide arms of specific dimensions, and recombining them.
    • 光子器件(100),其具有依赖于波长的透射特性或滤波器,包括:接收偏振光(1)和提供第一RESP一个分离器的偏振旋转器(11)。 第二波浪(2,3); 第一RESP。 连接到所述SPR用于传播第一RESP第二波导臂(12,13)。 第二偏振模式下的第一RESP的(TM,TE)。 第二波浪(2,3),第二偏振模(TE)与所述第一偏振模式(TM)不同; 和用于将所述第一传播分别偏振旋转器和组合器(14)。 第二波浪(2,3); worin所述第一和第二臂(12,13)的尺寸被选择为取消的上依赖于波长的特性的外部效应的影响。 以减少所述的灵敏度方法的集成光子器件,包括分束偏振光束(1),并通过特定的尺寸的两个波导臂中传播不同极性的光波(2,3),和重新组合。