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Stochastic amplitude fluctuation in coherent OTDR and a new technique for its reduction by stimulating synchronous optical frequency hopping
56
Citations
15
References
1997
Year
EngineeringOptical Transmission SystemWave OpticOptical Wireless CommunicationOptical PropertiesOptical CommunicationOptical SystemsRf Current PulseSynchronous Optical FrequencyDynamic RangePhotonicsPhysicsCoherent Detection OtdrSignal ProcessingCoherent OtdrCoherent ProcessStochastic Amplitude FluctuationOptoelectronicsWave Interference
The dynamic range of optical time-domain reflectometry (OTDR) can be extended by employing self-heterodyne coherent detection. However, with coherent detection OTDR (C-OTDR) there is a problem of amplitude fluctuation in the C-OTDR trace caused by (1) the fading noise resulting from the interference between the Rayleigh backscattered lights, (2) the polarization dependent fluctuation of the optical detection efficiency, and (3) the heterodyne detection efficiency fluctuation due to the relative phase change between the Rayleigh backscattered signals and the local oscillator (LO). This paper provides a stochastic description of the amplitude fluctuation using probability density functions and the calculated amplitude fluctuation with M integrations when reduction techniques are applied. We have found theoretically that it is difficult to reduce the amplitude fluctuation effectively by the optical frequency domain integration technique using the asynchronous optical frequency hopping of the source. This is because of an inclination increase in the C-OTDR trace which reduces the measurement accuracy. We propose a synchronous optical frequency hopping technique in which an RF current pulse is induced in the drive current of the laser diode (LD) during the LD temperature change. This effectively reduces the amplitude fluctuation without any increase in the inclination. The amplitude fluctuation for a 1 /spl mu/s pulse width is reduced experimentally to 1/7 that with the LD temperature stabilized. For 100 and 30 ns pulse widths, it is reduced to 1/11 of that with the LD temperature stabilized. These experimental results are in good agreement with the calculated ones.
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