Abstract
Optical passive ring-resonator gyro (OPRG) has been studied as a scheme to reduce the length of the sensing loop as well as to realize the linearity with wide dynamic range[1]- [6]. The OPRG needs a high coherence source to get a high finesse resonance. On the contrary, the fiber gyro requires the low coherence source to reduce the parasitic noises. Thus, the noise behavior in the OPRG is quite different from the fiber gyro. We have already discussed the behaviour of the noise sources in the OPRG, e.g., source coherence[1]-[2], Rayleigh backscattering[1]-[2], Kerr effect[3], and polarization problem[4].
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
