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

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.

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.

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 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, wherein the scattered light in a first propagation mode occurs when light in the first propagation mode is inputted into the multimode fiber;
• measure 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, wherein the scattered light in a second propagation mode occurs when light in the second propagation mode is inputted into the multimode fiber;
• and
• calculate 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.