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    • 4. 发明公开
    • Resonator fiber optic gyroscope utilizing laser frequency combs
    • Resonator-Glasfaser-Optikgyroskop,dasLaserfrequenzkämmebenutzt
    • EP2650644A2
    • 2013-10-16
    • EP13160955.4
    • 2013-03-25
    • Honeywell International Inc.
    • Sanders, Glen A.Strandjord, Lee K.Qiu, Tiequn
    • G01C19/72
    • G01C19/727G01C19/726G02B6/2934G02B6/29379
    • A resonator fiber optic gyroscope comprises a first light source having a first frequency comb spectrum, and a second light source having a second frequency comb spectrum. A first filter is in optical communication with the first light source and configured to pass a first frequency comb portion. A second filter is in optical communication with the second light source and configured to pass a second frequency comb portion. A resonator is in optical communication with the first and second filters. The free spectral range values of the first and second frequency comb portions are adjusted to be an odd integer multiple of the free spectral range value of the resonances of the resonator. The second frequency comb portion is spectrally separated apart from the first frequency comb portion by a multiple of the free spectral range value of the resonances plus a frequency value proportional to rotation rate.
    • 谐振器光纤陀螺仪包括具有第一频率梳状谱的第一光源和具有第二频率梳状谱的第二光源。 第一滤光器与第一光源光通信并且被配置为通过第一频率梳部分。 第二滤光器与第二光源光通信并被配置为通过第二频梳部分。 谐振器与第一和第二滤波器光学通信。 第一和第二频率梳状部分的自由光谱范围值被调整为谐振器的谐振的自由光谱范围值的奇数整数倍。 第二频率梳部分与第一频率梳部分分开,共振的自由频谱范围值加上与转速成比例的频率值的倍数。
    • 5. 发明公开
    • Systems and methods for driving an optical modulator
    • Systeme und Verfahren zum Antreiben eines optischen调制器
    • EP2463624A1
    • 2012-06-13
    • EP11192021.1
    • 2011-12-05
    • Honeywell International, Inc.
    • Smith, Douglas E.Armstrong, Steven G.Mead, Derek
    • G01C19/72
    • G01C19/721G01C19/726
    • Systems and methods for driving an optical modulator are provided. In one embodiment, a modulation drive circuit comprises: a balanced impedance network having a first and a second output generated from a first input, and a third and a fourth output generated from a second input, wherein the first and second outputs are balanced with one another, and the third and fourth outputs are balanced with one another; a first differential amplifier, wherein an inverting input of the first differential amplifier couples to the first output of the distribution network and a non-inverting input of the first differential amplifier couples to the third output of the distribution network; and a second differential amplifier, wherein an inverting input of the second differential amplifier couples to the fourth output of the distribution network and a non-inverting input of the second differential amplifier couples to the second output of the distribution network.
    • 提供了用于驱动光学调制器的系统和方法。 在一个实施例中,调制驱动电路包括:平衡阻抗网络,具有从第一输入产生的第一和第二输出以及从第二输入产生的第三和第四输出,其中所述第一和第二输出与一个 另一个,第三和第四个输出相互平衡; 第一差分放大器,其中所述第一差分放大器的反相输入耦合到所述分配网络的所述第一输出,并且所述第一差分放大器的非反相输入耦合到所述分配网络的第三输出; 以及第二差分放大器,其中所述第二差分放大器的反相输入耦合到所述分配网络的第四输出,并且所述第二差分放大器的非反相输入耦合到所述分配网络的第二输出。
    • 10. 发明公开
    • DIGITALER PHASENMODULATOR FÜR EINE FASEROPTISCHE EINRICHTUNG
    • 数字相位调制器光纤装置
    • EP1595111A1
    • 2005-11-16
    • EP04712523.2
    • 2004-02-19
    • LITEF GmbH
    • VOIGT, SvenSPAHLINGER, GünterNEWZELLA, Alfons
    • G01C19/72G02F1/01
    • G01C19/726G02F1/0115G02F1/0316G02F2201/122G02F2203/50
    • The invention relates to a digital phase modulator for a fiber-optic signal transmission or measuring device that has a predetermined total number m of electrodes (E0 to E11) of varying length that are disposed in parallel and at both sides of a light guiding path (L) in or on an optical substrate. The aim of the invention is to substantially increase the resolution of such a digital phase modulator. This aim is achieved by the method according to the invention and the corresponding system of electrodes which are based on the idea of dividing the electrodes up into two groups. A first group n of electrodes (E4 to E11) represents a macro-modulator having binary weighted and higher order electrodes with a length ratio of bn+1: bn = 2, whose longest electrode (E11) corresponds to the sum of lengths of all remaining electrodes of the overall modulator, while a second smaller group of n0 not-binary weighted and low order electrodes (E0 to E3) represents a micro-modulator. The smallest initial values are no longer produced by controlling individual electrodes of the micro-modulator but by calculating the difference between two larger electrodes each. Despite the comparatively short length of the phase modulator that would allow only for a resolution of 9 bits (electrode ratio of approximately 1:2-9) for technological reasons, the inventive subdivision into two different modulator concepts allows for a resolution in a value range of approximately 12 bits. The particular advantage is that it is no longer necessary to use a correction chart and if said chart, if available, fails, an emergency service with reduced resolution can be provided.