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    • 4. 发明授权
    • Systems and method to substantially mitigate AC stark shift effects in a sensor system
    • 基本上减轻传感器系统中的交流变换效应的系统和方法
    • US09229073B2
    • 2016-01-05
    • US13727926
    • 2012-12-27
    • Thad G. WalkerMichael D. BulatowiczMichael S. LarsenRobert C. GriffithPhilip R. Clark
    • Thad G. WalkerMichael D. BulatowiczMichael S. LarsenRobert C. GriffithPhilip R. Clark
    • G01R33/26G01C19/62
    • G01R33/26G01C19/62
    • One embodiment includes a sensor system. The system includes a cell system comprising a pump laser configured to generate a pump beam to polarize alkali metal particles enclosed within a sensor cell. The system also includes a detection system comprising a probe laser configured to generate a probe beam. The detection system can also be configured to calculate at least one measurable parameter based on characteristics of the probe beam passing through the sensor cell resulting from precession of the polarized alkali metal particles in response to an applied magnetic field. The system further includes an AC Stark shift control system configured to frequency-modulate the pump beam and to control a center frequency of a frequency-modulated pump beam based on the characteristics of the probe beam passing through the sensor cell to substantially stabilize and mitigate the effects of AC Stark shift on the at least one measurable parameter.
    • 一个实施例包括传感器系统。 该系统包括一个电池系统,该电池系统包括被配置成产生泵浦光束以使包围在传感器电池内的碱金属颗粒极化的泵浦激光器。 该系统还包括检测系统,其包括被配置为产生探测光束的探测激光器。 检测系统还可以被配置为基于由施加的磁场响应于偏振的碱金属颗粒的进动而导致通过传感器单元的探针束的特性来计算至少一个可测量的参数。 该系统还包括AC Stark变速控制系统,其配置成对泵浦波束进行频率调制,并且基于通过传感器单元的探测光束的特性来控制调频泵浦光束的中心频率,以基本上稳定和减轻 AC Stark移位对至少一个可测量参数的影响。
    • 7. 发明申请
    • GYROSCOPE SYSTEM MAGNETIC FIELD ERROR COMPENSATION
    • 陀螺仪系统磁场误差补偿
    • US20120191396A1
    • 2012-07-26
    • US13011530
    • 2011-01-21
    • Robert C. GriffithMichael S. LarsenMichael D. Bulatowicz
    • Robert C. GriffithMichael S. LarsenMichael D. Bulatowicz
    • G06F19/00
    • G01C19/62
    • One embodiment of the invention includes a nuclear magnetic resonance (NMR) gyroscope system. The system includes a gyro cell that is sealed to enclose an alkali metal vapor, a first gyromagnetic isotope, and a second gyromagnetic isotope. A magnetic field generator configured to generate a magnetic field that is provided through the gyro cell to cause the first and the second gyromagnetic isotopes to precess. A magnetic field error controller configured to measure an error associated with a magnitude of the magnetic field and to generate an error signal that is fed back to the magnetic field generator to maintain the magnetic field at a desired magnitude. The system further includes a mechanization processor configured to calculate a rotation angle about a sensitive axis of the NMR gyroscope system based on a measured precession angle of at least one of the first and second gyromagnetic isotopes and the error signal.
    • 本发明的一个实施例包括核磁共振(NMR)陀螺仪系统。 该系统包括密封以包围碱金属蒸气的陀螺仪单元,第一回旋磁同位素和第二回旋磁同位素。 磁场发生器被配置为产生通过陀螺仪单元提供的磁场,以使第一和第二回旋磁同位素进入。 磁场误差控制器被配置为测量与磁场的大小相关联的误差,并且产生反馈到磁场发生器以将磁场维持在期望的大小的误差信号。 该系统还包括机械化处理器,其被配置为基于所测量的第一和第二回旋磁同位素和误差信号中的至少一个的进动角来计算关于NMR陀螺仪系统的敏感轴的旋转角度。
    • 8. 发明授权
    • Optical accelerometer system
    • 光学加速度计系统
    • US09285390B2
    • 2016-03-15
    • US13907333
    • 2013-05-31
    • A. Douglas MeyerMichael D. BulatowiczMichael S. LarsenRobert C. Griffith
    • A. Douglas MeyerMichael D. BulatowiczMichael S. LarsenRobert C. Griffith
    • G01P15/08G01P15/093G01P15/18
    • G01P15/093G01P15/08G01P15/18
    • One embodiment includes an accelerometer system. The system includes a laser configured to emit an optical beam at a linear polarization. The system also includes an optical cavity system. The optical cavity system includes a mirror that is coupled to an accelerometer housing via a spring and is configured to reflect the optical beam. The optical cavity system also includes at least one photodetector configured to receive at least a portion of at least one of the optical beam and the reflected optical beam and to generate an acceleration signal that is indicative of motion of the mirror resulting from an external acceleration acting upon the accelerometer housing. The system further includes an acceleration processor configured to calculate a magnitude of the external acceleration based on the acceleration signal.
    • 一个实施例包括加速度计系统。 该系统包括被配置为以线偏振发射光束的激光器。 该系统还包括光腔系统。 光学腔系统包括经由弹簧耦合到加速度计壳体的反射镜,并被配置为反射光束。 光腔系统还包括至少一个光电检测器,其被配置为接收光束和反射光束中的至少一个的至少一部分,并且产生指示由外部加速度作用产生的反射镜的运动的加速度信号 在加速度计外壳上。 该系统还包括加速度处理器,该加速度处理器被配置为基于加速度信号来计算外部加速度的大小。
    • 9. 发明授权
    • Gyroscope system magnetic field error compensation
    • 陀螺仪系统磁场误差补偿
    • US08600691B2
    • 2013-12-03
    • US13011530
    • 2011-01-21
    • Robert C. GriffithMichael S. LarsenMichael D. Bulatowicz
    • Robert C. GriffithMichael S. LarsenMichael D. Bulatowicz
    • G01C17/38G01V3/00
    • G01C19/62
    • One embodiment of the invention includes a nuclear magnetic resonance (NMR) gyroscope system. The system includes a gyro cell that is sealed to enclose an alkali metal vapor, a first gyromagnetic isotope, and a second gyromagnetic isotope. A magnetic field generator configured to generate a magnetic field that is provided through the gyro cell to cause the first and the second gyromagnetic isotopes to precess. A magnetic field error controller configured to measure an error associated with a magnitude of the magnetic field and to generate an error signal that is fed back to the magnetic field generator to maintain the magnetic field at a desired magnitude. The system further includes a mechanization processor configured to calculate a rotation angle about a sensitive axis of the NMR gyroscope system based on a measured precession angle of at least one of the first and second gyromagnetic isotopes and the error signal.
    • 本发明的一个实施例包括核磁共振(NMR)陀螺仪系统。 该系统包括密封以包围碱金属蒸气的陀螺仪单元,第一回旋磁同位素和第二回旋磁同位素。 磁场发生器被配置为产生通过陀螺仪单元提供的磁场,以使第一和第二回旋磁同位素进入。 磁场误差控制器被配置为测量与磁场的大小相关联的误差,并且产生反馈到磁场发生器以将磁场维持在期望的大小的误差信号。 该系统还包括机械化处理器,其被配置为基于所测量的第一和第二回旋磁同位素和误差信号中的至少一个的进动角来计算关于NMR陀螺仪系统的敏感轴的旋转角度。