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Patent

Laser fiber optic gyroscope having phase modulation

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TLDR
In this paper, a non-reciprocal phase modulation is introduced between the clockwise (CW) and counterclockwise (CCW) beams at a modulation frequency (f), and the detected signal is demodulated by mixing it with a reference signal at the same frequency and stepping the phase of the signal through successive increments of 90°, thereby to determine the inphase and quadrature components for each frequency monitored.
Abstract
In a laser gyroscope, a non-reciprocal phase modulation is introduced between the clockwise (CW) and counterclockwise (CCW) beams at a modulation frequency (f). The CW and CCW beams are combined on a detector and the intensity of the output is observed at the fundamental frequency (f) and the higher harmonics (e.g. 2f, 4f). At each frequency, the detected signal is demodulated by mixing it with a reference signal at the same frequency and stepping the phase of the signal through successive increments of 90°, thereby to determine the in-phase and quadrature components for each frequency monitored.

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Citations
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Decreasing the effects of linear birefringence in a fiber-optic sensor by use of berry's topological phase

TL;DR: In this paper, the pitch angle of the fiber was selected to result in a phase shift due to Berry's phase of circularly polarized light propagating through the fiber, and the desired pitch angle may be approximately 60°.
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Apparatus and method for electronic RIN reduction in fiber-optic sensors utilizing filter with group delay

TL;DR: In this article, a method for reducing RIN noise in optical sensors, in particular fiber-optic sensors, is described, where the optical sensor produces a sensor output signal representing a physical quantity to be measured and also contains a first noise component, which is detected by a first detector.
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Apparatus and method for electronic RIN reduction in fiber-optic sensors

TL;DR: In this article, a method for reducing RIN noise in optical sensors, in particular fiber-optic sensors, is described, where the optical sensor produces a sensor output signal representing a physical quantity to be measured and also contains a first noise component, which is detected by a first detector.
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TL;DR: In this article, a RFOG consisting of a reference laser, a first laser source, a second laser source and a sensing resonator coupled to the first and second laser sources is defined.
References
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Patent

Optical fiber measuring device, gyrometer, central navigation and stabilizing system

TL;DR: In this article, the phase difference between two waves in a SAGNAC ring interferometer was modulated in such a way that the gain of the channel for controlling the modulation was kept constant by producing a signal depending on the said gain.
Patent

Fiber optic gyro stabilized by harmonic components of detected signal

Kenichi Okada
TL;DR: In this article, a phase modulator is inserted in one end of the circular optical path, by which the light waves are phase modulated, and the intensity of the interference light is detected, as an electric signal, by a photodetector.
Patent

Fiber optical rotation sensor utilizing the Sagnac phase difference

TL;DR: In this paper, a laser wave omitted from a laser diode is guided into a one directional optical coupler and is splitted into two laser waves by the coupler, and one of the splitted interference laser waves is then converted into an electric signal by the photodetector.
Patent

Switched state fiber optic gyroscope

TL;DR: In this paper, an improved fiber optic gyroscope with a substantial improvement in dynamic range and scale factor stability over a basic fiber-optic gyroswope is disclosed.
Patent

Method and device for detecting propagation time variations in a ring interferometer and application thereof to wave length control

TL;DR: In this paper, a method and corresponding device are provided for detecting the propagation time variations in the ring of an interferometer and includes phase modulation of the contrarotating waves travelling through the ring by means of assymetric square waves at a period twice the initial propagation time.