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    • 4. 发明授权
    • Reconfigurable liquid metal fiber optic mirror
    • 可重构液态金属光纤镜
    • US09274271B2
    • 2016-03-01
    • US14027262
    • 2013-09-16
    • Ross SchermerCarl A. VillarruelFrank BucholtzColin McLaughlin
    • Ross SchermerCarl A. VillarruelFrank BucholtzColin McLaughlin
    • G02B6/02G02B6/032G02B6/28
    • G02B6/02295G02B6/02328G02B6/02385G02B6/0239G02B6/032G02B6/2861H04B2210/006
    • A true time delay system for optical signals includes a hollow core optical waveguide, a droplet of reflective liquid metal disposed in the hollow core, and an actuator coupled to a first end of the waveguide to move the droplet longitudinally within the hollow core. In one example, the waveguide is a hollow core photonic bandgap fiber. In one example, the actuator is a pressure actuator that introduces or removes gas into the core. Light enters the optical fiber, is transmitted through the fiber toward the reflective surface of the droplet, and is reflected back through the fiber and exits at the same end of the photonic bandgap optical fiber that it entered. The fiber optic device can provide a continuously-variable optical path length of over 3.6 meters (corresponding to a continuously-variable true-time delay of over 12 ns, or 120 periods at a 10 GHz modulation frequency), with negligible wavelength dependence across the C and L bands.
    • 用于光学信号的真实时间延迟系统包括中空芯光波导,设置在中空芯中的反射液体金属液滴,以及耦合到波导的第一端的致动器,以在中空芯内纵向移动液滴。 在一个示例中,波导是空心芯光子带隙光纤。 在一个示例中,致动器是将气体引入或去除到芯中的压力致动器。 光进入光纤,通过光纤传输到液滴的反射表面,并通过光纤反射回来,并在光纤带入光纤的同一端退出。 光纤设备可以提供超过3.6米的连续可变光路长度(对应于超过12ns的连续可变的真实时间延迟,或在10GHz调制频率下的120个周期),其中波长依赖性可忽略不计 C和L波段。
    • 6. 依法登记的发明
    • Interferometric fiber optic sensor configuration with pump-induced phase
carrier
    • 干涉光纤传感器配置与泵浦相载波
    • USH1436H
    • 1995-05-02
    • US959584
    • 1992-10-13
    • Alan D. KerseyCarl A. Villarruel
    • Alan D. KerseyCarl A. Villarruel
    • G01D5/353G01B9/02
    • G01D5/35303
    • An interferometric fiber optic sensor and method are provided for controlling the optical phase of a fiber interferometer by an optically induced change in the refractive index for one arm of the fiber interferometer and providing a passive all-optical phase shift interrogation in response to this dependency on the optically induced change in the refractive index. The interferometric fiber optic sensor includes a laser source for generating light at a first predetermined wavelength, a fiber interferometer coupled to the laser source and having first and second fiber arms with a predetermined optical path difference between the fiber arms, a predetermined one of the first and second fiber arms being doped with an element for introducing an optically adjustable absorption spectrum, and a pump laser coupled to the predetermined fiber arm for generating light at a second predetermined wavelength so that an effective index for a guided mode in the predetermined fiber arm and a phase delay of the light passing through the fiber interferometer are changed. As a result, the interferometric fiber optic sensor and method allows the phase interrogation of the fiber interferometer by using a passive all-optical approach based on a pump induced refractive index change in the doped fiber arm so that balanced all fiber interferometer elements are used as sensors for eliminating laser induced phase noise.
    • 7. 发明授权
    • Waveguide-binding sensor for use with assays
    • 用于测定的波导结合传感器
    • US5061857A
    • 1991-10-29
    • US610895
    • 1990-11-09
    • Richard B. ThompsonCarl A. Villarruel
    • Richard B. ThompsonCarl A. Villarruel
    • A61B5/00G01N21/64G01N21/77
    • G01N21/648A61B5/1459G01N21/6428G01N21/7703G01N2021/6432G01N2021/6434
    • An optical waveguide-binding sensor which increases sensor sensitivity to fluorescence detection during assays of liquids based on adjustments in the V number along the optical waveguide. The sensing waveguide includes a mode converting section where the V number of the wavguide gradually increases from the distal sensing end of the mode converting section to the proximal end of the mode converting section. The gradually change in V number can be accomplished by either gradually inwardly tapering waveguide along the sensor portion from the proximal end, or by gradually varying the dopant concentration along the sensing portion. The sensor tapers in diameter to change the V number along the distal end of the optical waveguide. The present invention increases the efficiency of fluorescence detection by converting weakly-guided high-order modes of fluorescence radiation at the distal end into lower-order modes at the proximal and increases the efficiency of fluorescent excitation by converting low order mode entering the proximal end into weakly-guided high order modes at the sensing end. At the sensing end, these weakly guided modes cn strengthen the evanescent excitation wave.
    • 一种光波导结合传感器,其基于沿着光波导的V数的调节,增加了液体测定期间对荧光检测的灵敏度。 感测波导包括模式转换部分,其中W形导体的V数从模式转换部分的远端感测端逐渐增加到模式转换部分的近端。 V数的逐渐变化可以通过从近端沿着传感器部分逐渐向内逐渐变细的波导,或者沿着感测部分逐渐改变掺杂剂浓度来实现。 传感器的直径逐渐变细,沿着光波导的远端改变V数。 本发明通过将远端的弱引导高阶模式的近端的高阶模式转换为近端的低阶模式来提高荧光检测的效率,并且通过将进入近端的低阶模式转换成低频模式来提高荧光激发的效率 弱导向高阶模式在感应端。 在感测端,这些弱引导模式cn加强了消逝激发波。
    • 8. 发明申请
    • Reconfigurable Liquid Metal Fiber Optic Mirror
    • 可重构液态金属光纤镜
    • US20140105554A1
    • 2014-04-17
    • US14027262
    • 2013-09-16
    • Ross SchermerCarl A. VillarruelFrank BucholtzColin McLaughlin
    • Ross SchermerCarl A. VillarruelFrank BucholtzColin McLaughlin
    • G02B6/02G02B6/032
    • G02B6/02295G02B6/02328G02B6/02385G02B6/0239G02B6/032G02B6/2861H04B2210/006
    • A true time delay system for optical signals includes a hollow core optical waveguide, a droplet of reflective liquid metal disposed in the hollow core, and an actuator coupled to a first end of the waveguide to move the droplet longitudinally within the hollow core. In one example, the waveguide is a hollow core photonic bandgap fiber. In one example, the actuator is a pressure actuator that introduces or removes gas into the core. Light enters the optical fiber, is transmitted through the fiber toward the reflective surface of the droplet, and is reflected back through the fiber and exits at the same end of the photonic bandgap optical fiber that it entered. The fiber optic device can provide a continuously-variable optical path length of over 3.6 meters (corresponding to a continuously-variable true-time delay of over 12 ns, or 120 periods at a 10 GHz modulation frequency), with negligible wavelength dependence across the C and L bands.
    • 用于光学信号的真实时间延迟系统包括中空芯光波导,设置在中空芯中的反射液体金属液滴,以及耦合到波导的第一端的致动器,用于在中空芯内纵向移动液滴。 在一个示例中,波导是空心芯光子带隙光纤。 在一个示例中,致动器是将气体引入或去除到芯中的压力致动器。 光进入光纤,通过光纤传输到液滴的反射表面,并通过光纤反射回来,并在光纤带入光纤的同一端退出。 光纤设备可以提供超过3.6米的连续可变光路长度(对应于超过12ns的连续可变的真实时间延迟,或在10GHz调制频率下的120个周期),其中波长依赖性可忽略不计 C和L波段。
    • 10. 发明授权
    • Polarization-preserving single mode fiber coupler
    • 极化保护单模光纤耦合器
    • US4612028A
    • 1986-09-16
    • US785107
    • 1985-10-07
    • Moges AbebeWilliam K. BurnsCarl A. Villarruel
    • Moges AbebeWilliam K. BurnsCarl A. Villarruel
    • G02B6/28C03B23/20
    • G02B6/2843G02B6/2835
    • A polarization-preserving single mode fiber coupler, fabricated by a method which does not require mutually aligning the fiber polarization axes provided the actual misalignment angle is not close to 90.degree.. The protective jackets from two or more polarization-preserving single mode birefringent fibers are partially removed and the fibers are twisted around each other to bring them into contact over the jacketless region and provide a coupling length that is large compared to the birefringent beat length of the fibers. Next, the cladding layers of the fibers in the contacting region are partially etched without degrading the birefringent beat length over their coupling length. Then, the etched region is heated to the softening point of the fibers while axial tension is applied to taper and fuse the etched region until a desired coupling of the fibers is achieved. Finally, a mechanical supporting structure is added to the tapered and fused region of the fibers.
    • 通过不需要相互对准提供实际偏移角的光纤偏振轴的方法制造的偏振保持单模光纤耦合器不接近90°。 来自两个或更多个偏振保持单模双折射光纤的保护套被部分地去除,并且纤维彼此扭曲以使它们在无夹套区域上接触,并提供与双折射拍子长度相比大的耦合长度 纤维。 接下来,接触区域中的纤维的包覆层被部分地蚀刻,而不会使双折射拍子长度在其耦合长度上降低。 然后,将蚀刻的区域加热到纤维的软化点,同时施加轴向张力来锥形并熔化被蚀刻的区域,直到实现所需的纤维的耦合。 最后,机械支撑结构被添加到纤维的锥形和熔融区域。