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    • 81. 发明授权
    • Optical image processing using minimum phase functions
    • 使用最小相位函数的光学图像处理
    • US08082117B2
    • 2011-12-20
    • US12623322
    • 2009-11-20
    • Aydogan OzcanMichel J. F. DigonnetGordon S. Kino
    • Aydogan OzcanMichel J. F. DigonnetGordon S. Kino
    • G06F17/14G01N21/00
    • G06E3/003G01J3/45G01J11/00
    • A method utilizes an optical image processing system. The method includes providing a measured magnitude of the Fourier transform of a complex transmission function of an object or optical image. The method further includes providing an estimated phase term of the Fourier transform of the complex transmission function. The method further includes multiplying the measured magnitude and the estimated phase term to generate an estimated Fourier transform of the complex transmission function. The method further includes calculating an inverse Fourier transform of the estimated Fourier transform, wherein the inverse Fourier transform is a spatial function. The method further includes calculating an estimated complex transmission function by applying at least one constraint to the inverse Fourier transform.
    • 一种方法利用光学图像处理系统。 该方法包括提供物体或光学图像的复数传输函数的傅里叶变换的测量幅度。 该方法还包括提供复传输函数的傅立叶变换的估计相位项。 该方法还包括将测量的幅度和估计的相位项相乘以产生复数传输函数的估计傅里叶变换。 该方法还包括计算傅立叶逆变换的傅立叶逆变换,其中逆傅里叶变换是空间函数。 该方法还包括通过对傅里叶逆变换应用至少一个约束来计算估计的复传输函数。
    • 84. 发明授权
    • Optical sensor utilizing hollow-core photonic bandgap fiber with low phase thermal constant
    • 光学传感器利用空心光子带隙光纤具有低相位热常数
    • US07619743B2
    • 2009-11-17
    • US11770660
    • 2007-06-28
    • Michel J. F. DigonnetHyang Kyun KimVinayak DanguiGordon S. Kino
    • Michel J. F. DigonnetHyang Kyun KimVinayak DanguiGordon S. Kino
    • G01C19/72
    • G01D5/3538G01C19/721G01D5/35322G02B6/02328
    • An optical sensor includes a directional coupler comprising at least a first port, a second port, and a third port. The first port is in optical communication with the second port and with the third port such that a first optical signal received by the first port is split into a second optical signal that propagates to the second port and a third optical signal that propagates to the third port. The optical sensor further includes a photonic bandgap fiber having a hollow core and an inner cladding generally surrounding the core. The photonic bandgap fiber is in optical communication with the second port and with the third port. The second optical signal and the third optical signal counterpropagate through the photonic bandgap fiber and return to the third port and the second port, respectively. The photonic bandgap fiber has a phase thermal constant S less than 8 parts-per-million per degree Celsius.
    • 光学传感器包括至少包括第一端口,第二端口和第三端口的定向耦合器。 第一端口与第二端口和第三端口光通信,使得由第一端口接收的第一光信号被分裂成传播到第二端口的第二光信号和传播到第三端口的第三光信号 港口。 光学传感器还包括具有中空芯和通常围绕芯的内包层的光子带隙光纤。 光子带隙光纤与第二端口和第三端口光通信。 第二光信号和第三光信号通过光子带隙光纤反向传播并分别返回到第三端口和第二端口。 光子带隙光纤的相位热常数S小于每摄氏摄氏度百万分之八。
    • 87. 发明授权
    • Fast, environmentally-stable fiber switches using a Sagnac interferometer
    • US06584241B2
    • 2003-06-24
    • US10072559
    • 2002-02-08
    • Monica K. DavisMichel J. F. Digonnet
    • Monica K. DavisMichel J. F. Digonnet
    • G02F1295
    • G02F1/3519
    • A fast, environmentally-stable fiber switch uses a Sagnac interferometer having an active fiber portion located asymmetrically in the loop of the interferometer. A pump pulse is applied to the interferometric loop and acts upon the active fiber portion to cause a change in its refractive index either by a thermal effect or by a non-thermal nonlinear effect. Because the active fiber portion is located asymmetrically in the loop, the change in refractive index of the active fiber portion is seen by the clockwise propagating light signal and the counterclockwise propagating light signal at different times, thus causing a temporary difference in the phase changes experienced by the two counterpropagating light signals. The temporary difference in the phase changes causes the two light signals to combine constructively at a switched output port of the input/output coupler of the interferometric loop until the phase changes of the two signals are again the same, at which time the signals combine at an unswitched output port of the coupler. The on-time of the switch is set primarily by the length of the Sagnac loop, and the fall time, which is caused by the Sagnac architecture, can be fast, even with a relatively slow active fiber.
    • 89. 发明授权
    • Gain flattening with nonlinear sagnac amplifiers
    • US06466364B1
    • 2002-10-15
    • US10060868
    • 2002-01-29
    • Benjamin J. VakocMichel J. F. Digonnet
    • Benjamin J. VakocMichel J. F. Digonnet
    • H01S300
    • H04B10/294G02F1/3519H01S3/06754H01S3/1302H01S2301/04H01S2301/06H04B10/2935
    • An apparatus and a method provide gain flattening in communications systems wherein a large number of optical signals at different wavelengths must be amplified while maintaining signal power within an acceptable range. Because of differences in gain of typical optical amplifiers as a function of wavelength and input power, the signals at different wavelengths are not amplified by the same amounts. Thus, when amplified multiple times, certain signals tend to become severely attenuated to the point of being no longer useable. The present gain flattening apparatus and method cause signals having higher gain-power products to be attenuated by a greater amount in response to Kerr-induced phase shifting such that after multiple stages of amplification, all the signal powers converge toward a small range of acceptable output powers. The apparatus provides amplification, multiple times, of a series of signals with a plurality of wavelengths covering a very wide spectral range, while maintaining the power of all the signals within a small range. The spread of this signal power range is robust against changes in the signal power, against changes in the number of signals, and, to some degree, against changes in the amplifier's pump power. The apparatus design is also robust against manufacturing changes in the parameters of the apparatus' components. The apparatus and invention are preferably implemented as multiple nonlinear Sagnac amplifiers having erbium-doped fiber amplifiers positioned asymmetrically in an interferometer loop.
    • 90. 发明授权
    • Electrostrictive fiber modulators
    • 电致伸缩纤维调节剂
    • US06385354B1
    • 2002-05-07
    • US09259832
    • 1999-03-01
    • Michel J. F. DigonnetAlice LiuGordon S. Kino
    • Michel J. F. DigonnetAlice LiuGordon S. Kino
    • G02F101
    • G02F1/0134G02F1/3136
    • An apparatus modulates the phase of an optical signal. The apparatus includes an optical medium for propagating the optical signal. At least one electrode is positioned in proximity with the medium. The electrode induces an electric field within the medium in response to an AC voltage to produce variations in the index of refraction of the optical medium through the electrostrictive effect. Preferably, the phase of the optical signal is modulated such that polarization components of the optical signal parallel to and orthogonal to the electric field experience an equal phase shift. In certain embodiments, a DC voltage is supplied to the optical medium. Alternatively, the DC voltage within the optical medium may arise from (or be enhanced by) poling the optical medium. Certain embodiments of the present invention include two electrodes positioned on opposite sides of the optical medium. The apparatus is advantageously used in an interferometer to form a device that modulates the amplitude of the optical signal. The apparatus may also be used in an interferometer to form an optical switching device.
    • 一种装置调制光信号的相位。 该装置包括用于传播光信号的光学介质。 至少一个电极定位在介质附近。 电极响应于AC电压在介质内引起电场,以通过电致伸缩效应产生光学介质的折射率的变化。 优选地,调制光信号的相位,使得平行于和与电场正交的光信号的偏振分量经历相等的相移。 在某些实施例中,DC电压被提供给光学介质。 或者,光学介质内的DC电压可以由(或通过)光学介质极化而产生。 本发明的某些实施例包括位于光学介质的相对侧上的两个电极。 该装置有利地用于干涉仪中以形成调制光信号幅度的装置。 该装置还可用于干涉仪中以形成光开关装置。