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Fiber-optic distributed measurement of polarization beat length using slope-assisted Brillouin optical correlation-domain reflectometry

Heeyoung Lee 30870787 Kohei Noda Kentaro Nakamura 20242315 Yosuke Mizuno 30630818 横浜国立大学

2020.10.11

概要

A cost-effective method for estimating the Brillouin frequency shift (BFS) of the whole sensing fiber without using an electrical spectrum analyzer is developed. The Brillouin gain spectrum is down-converted and low-pass-filtered, and its total transmitted power is used to estimate the BFS. The strain dynamic range of this method is experimentally shown to be double the value of a conventional slope-assisted method.

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参考文献

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Figure Captions

Figure 1 Experimental setup of SA-BOCDR-based beat length measurement. EDFA,

erbium-doped fiber amplifier; ESA, electrical spectrum analyzer; FUT, fiber under test;

OSC, oscilloscope; PC, polarization controller; PD, photo diode; PSCR, polarization

scrambler.

Figure 2 Measurement of spectral power distributions. (a) structure of the FUT, R=10.5

cm; (b) power distribution along the FUT, R = 10.5 cm; (c) structure of the FUT, R=7.5 cm;

(d) power distribution along the FUT, R = 7.5 cm; (e) structure of the FUT, R=3.4 cm; (f)

power distribution along the FUT, R = 3.4 cm.

Figure 3 Calculated PSDs (log scale) when R was (a) 10.5 cm; (b) 7.5 cm; (c) 3.4 cm. The

insets show their magnified views around the peaks (linear scale).

Figure 4 Measured beat length plotted as a function of the mandrel radius. The solid curve

is a theoretical trend.

Figure 5 Demonstration of distributed beat length measurement. (a) Structure of the FUT

comprising two sections wound on mandrels with radii (10.5 cm and 3.4 cm). (b) Spectral

power distribution along the FUT with R = 10.5 cm (90–180-m section) and R = 3.4 cm

(180–195-m section). (c) Its magnified view in the 180–195-m section.

Figures

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