Measurement method, measurement device, and non-transitory recording medium

Patent metadata

Field	Value
Publication number	US-10760993-B2
Application number	US-201716329130-A
Country	US
Kind code	B2
Filing date	May 1, 2017
Priority date	Aug 31, 2016
Publication date	Sep 1, 2020
Grant date	Sep 1, 2020

Abstract

A measurement method for measuring an effective refractive index difference between two propagation modes of a multimode fiber is provided. The method includes: measuring a first Brillouin frequency shift ν1 by specifying a frequency having a lowest-frequency peak out of peaks in a first frequency spectrum of scattered light in a first propagation mode; measuring a second Brillouin frequency shift ν2 by specifying a frequency having a lowest-frequency peak out of peaks in a second frequency spectrum of scattered light in a second propagation mode; and calculating an effective refractive index difference Δneff in accordance with Δneff=(ν1−ν2)/(2kVL) with use of the first Brillouin frequency shift ν1, the second Brillouin frequency shift ν2, a predetermined wave number k of light in a vacuum, and a predetermined constant VL.

First claim

The invention claimed is:

1. A measurement method for measuring an effective refractive index difference between two propagation modes of a multimode fiber, the method comprising:
measuring a first Brillouin frequency shift ν 1 by specifying a frequency having a lowest-frequency peak out of peaks in a first frequency spectrum of scattered light in a first propagation mode, wherein the scattered light in a first propagation mode occurs when light in the first propagation mode is inputted into the multimode fiber;
measuring a second Brillouin frequency shift ν 2 by specifying a frequency having a lowest-frequency peak out of peaks in a second frequency spectrum of scattered light in a second propagation mode, wherein the scattered light in a second propagation mode occurs when light in the second propagation mode is inputted into the multimode fiber; and
calculating an effective refractive index difference Δn eff in accordance with Δn eff =(ν 1 −ν 2 )/(2kV L ) with use of the first Brillouin frequency shift ν 1 , the second Brillouin frequency shift ν 2 , a predetermined wave number k of light in a vacuum, and a predetermined constant V L .

2. The measurement method as set forth in claim 1 , wherein:
the measuring of the first Brillouin frequency shift ν 1 comprises measuring longitudinal distribution of the first Brillouin frequency shift ν 1 in the multimode fiber with a BOTDR (Brillouin Optical-Fiber Time Domain Reflectometry) or a BOTDA (Brillouin Optical-Fiber Time Domain Analysis);
the measuring of the second Brillouin frequency shift ν 2 comprises measuring longitudinal distribution of the second Brillouin frequency shift ν 2 in the multimode fiber with the BOTDR; and
the calculating of the effective refractive index difference Δneff comprises calculating longitudinal distribution of the effective refractive index difference Δn eff in the multimode fiber with the longitudinal distribution of the first Brillouin frequency shift ν 1 and the longitudinal distribution of the second Brillouin frequency shift ν 2 .

3. The measurement method as set forth in claim 1 , wherein:
the measuring of the first Brillouin frequency shift ν 1 comprises specifying a frequency that has a peak of a single Lorentzian function that best approximates the first frequency spectrum or of a Lorentzian function whose peak is in a lowest frequency side among a plurality of Lorentzian functions that form a sum that best approximates the first frequency spectrum; and
the measuring of the second Brillouin frequency shift ν 2 comprises specifying a frequency that has a peak of a single Lorentzian function that best approximates the second frequency spectrum or of a Lorentzian function whose peak is in a lowest frequency side among a plurality of Lorentzian functions that form a sum that best approximates the second frequency spectrum.

4. The measurement method as set forth in claim 1 , wherein:
the first propagation mode is an LP01 mode;
the second propagation mode is an LP11 mode;
the first Brillouin frequency shift ν 1 is a Brillouin frequency shift ν LP01→L01→LP01 corresponding to a scattering process in which scattered light in the LP01 mode occurs from light in the LP01 mode via an acoustic mode L01;
the second Brillouin frequency shift ν 2 is a Brillouin frequency shift ν LP11→L01→LP11 corresponding to a scattering process in which scattered light in the LP11 mode occurs from light in the LP11 mode via the acoustic mode L01; and
the constant V L is an approximate value of a longitudinal phase velocity V L01 of the acoustic mode L01.

5. A measurement device for measuring an effective refractive index difference between two propagation modes of a multimode fiber, the device comprising:
a BOTDR (Brillouin Optical-Fiber Time Domain Reflectometry) that comprises an output port and an input port;
a circulator that comprises a first port, a second port, and a third port, wherein the first port connects the output port of the BOTDR, and the third port connects to the input port of the BOTDR;
first and second single-mode fibers that each comprise an input end and an output end, wherein one of the input end of the first single-mode fiber and the input end of the second single-mode fiber connects to the second port of the circulator; and
a mode coupler that comprises a first input port, a second input port, and an output port, wherein the first input port of the mode coupler connects to the output end of the first single-mode fiber, the second input port of the mode coupler connects to the output end of the second single-mode fiber, the output port of the mode coupler connects to an input end of the multimode fiber, and the mode coupler couples a propagation mode in the first single-mode fiber with a first propagation mode in the multimode fiber and couples a propagation mode in the second single-mode fiber with a second propagation mode in the multimode fiber.

6. A measurement device for measuring an effective refractive index difference between two propagation modes which a multimode fiber has, the device comprising:
a BOTDA (Brillouin Optical-Fiber Time Domain Analysis) that comprises a pump light output port and a probe light input port;
a circulator that comprises a first port, a second port, and a third port, wherein the first port of the circulator connects to the pump light output port of the BOTDA, and the third port connects to the probe light input port of the BOTDA;
first and second single-mode fibers that each comprise an input end and an output end, wherein one of the input end of the first single-mode fiber and the input end of the second single-mode fiber connects to the second port of the circulator;
a first mode coupler that comprises a first input port, a second input port, and an output port, wherein the first input port of the first mode coupler connects to the output end of the first single-mode fiber, the second input port of the first mode coupler connects to the output end of the second single-mode fiber, the output port of the first mode coupler connects to an input end of the multimode fiber, and the first mode coupler couples a propagation mode in the first single-mode fiber with a first propagation mode in the multimode fiber and couples a propagation mode in the second single-mode fiber with a second propagation mode in the multimode fiber;
third and fourth single-mode fibers that each comprise an input end and an output end, wherein one of the output end of the third single-mode fiber and the output end of the fourth single-mode fiber connects to the probe light input port of the BOTDA; and
a second mode coupler that comprises an input port, a first output port, and a second output port, wherein the input port of the second mode coupler connects to an output end of the multimode fiber, the first output port of the second mode coupler connects to the input end of the third single-mode fiber, the second output port of the second mode coupler connects to the input end of the fourth single-mode fiber, and the second mode coupler couples the first propagation mode in the multimode fiber with a propagation mode in the third single-mode fiber and couples the second propagation mode in the multimode fiber with a propagation mode in the second single-mode fiber.

7. A non-transitory recording medium storing a computer-readable program for measuring an effective refractive index difference between two propagation modes of a multimode fiber, wherein the computer-readable program causes a computer to:
measure a first Brillouin frequency shift ν 1 by specifying a frequency having a lowest-frequency peak out of peaks in a first frequency spectrum of scattered light in a first propagation mode, wherein the scattered light in a first propagation mode occurs when l

Assignees

• Fujikura Ltd
• National Univ Corporation Shimane Univ

Inventors

• Maruyama Ryo
• Kuwaki Nobuo
• Ito Fumihiko

Classifications

• G01M11/3145 Primary

  Details of the optoelectronics or data analysis · CPC title

• G01M11/33

  with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face · CPC title

• G01M11/39

  in which light is projected from both sides of the fiber or waveguide end-face · CPC title

• G01D5/35364

  using inelastic backscattering to detect the measured quantity, e.g. using Brillouin or Raman backscattering · CPC title

• G01D5/35358

  using backscattering to detect the measured quantity · CPC title