IP Library Granted Patent US 10,073,006
Granted Patent B2
US 10,073,006 · App. 15/130,287 · Granted Sep 11, 2018

Brillouin and rayleigh distributed sensor

Inventor: Vincent Lecoeuche (Tarentaise, FR)
Assignee: VIAVI SOLUTIONS INC.
G01M11/3181G01D5/35358G01D5/35361G01D5/35364G01M11/3127G01M11/3172
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Quick Facts
Patent No.
US 10,073,006
App. No.
15/130,287
Filed
Apr 15, 2016
Granted
Sep 11, 2018
Kind
B2
Art Unit
2886
USPC
356/73.1
Abstract

According to examples, a Brillouin and Rayleigh distributed sensor may include a first laser source to emit a first laser beam, and a second laser source to emit a second laser beam. A photodiode may acquire a beat frequency between the two laser beams. The beat frequency may be used to maintain a predetermined offset frequency shift between the two laser beams. A modulator may modulate the first laser beam. The modulated first laser beam is to be injected into a device under test (DUT). A coherent receiver may acquire a backscattered signal from the DUT. The backscattered signal results from the modulated first laser beam injected into the DUT. The coherent receiver may use the second laser beam as a local oscillator to determine Brillouin and Rayleigh traces with respect to the DUT based on the predetermined offset frequency shift.

Claims (53)

1. A Brillouin and Rayleigh distributed sensor comprising:

a first laser source to emit a first laser beam;

a second laser source to emit a second laser beam;

a photodiode to acquire a beat frequency between the first laser beam and the second laser beam, wherein the beat frequency is used to maintain a predetermined offset frequency shift between the first laser beam and the second laser beam, wherein the predetermined offset frequency shift is relative to a predetermined frequency of either the first laser beam or the second laser beam;

a modulator to modulate the first laser beam, wherein the modulated first laser beam is to be injected into a device under test (DUT);

a coherent receiver to acquire a backscattered signal from the DUT, wherein the backscattered signal results from the modulated first laser beam injected into the DUT, and wherein the coherent receiver is to use the second laser beam as a local oscillator to determine Brillouin and Rayleigh traces with respect to the DUT based on the predetermined offset frequency shift between the first laser beam and the second laser beam by further using

a first polarization beam splitter (PBS) of the coherent receiver to

receive the second laser beam, and

divide the second laser beam into two different polarization states including a first polar state and a second polar state, and

a second PBS of the coherent receiver to

receive the backscattered signal, and

divide the backscattered signal into two different polarization states including a first polar state and a second polar state that are the same as the first and second polar states of the second laser beam, wherein a divided portion of the backscattered signal corresponding to the first polar state is to be mixed with the second laser beam at the first polar state, and a divided portion of the backscattered signal corresponding to the second polar state is to be mixed with the second laser beam at the second polar state to determine the Brillouin and Rayleigh traces with respect to the DUT.

2. The Brillouin and Rayleigh distributed sensor of claim 1 , wherein the predetermined offset frequency shift for determination of the Brillouin trace is approximately 10.8 GHz.

3. The Brillouin and Rayleigh distributed sensor of claim 1 , wherein the predetermined offset frequency shift for determination of the Brillouin trace is selected from a range of approximately 10.0 GHz to approximately 13.0 GHz.

4. The Brillouin and Rayleigh distributed sensor of claim 1 , wherein the predetermined offset frequency shift for determination of the Rayleigh trace is selected from a range of approximately 100.0 KHz to approximately 1.0 GHz.

5. The Brillouin and Rayleigh distributed sensor of claim 1 , wherein the DUT is an optical fiber.

6. A method for Brillouin trace and Rayleigh trace determination, the method comprising:

maintaining a predetermined offset frequency shift between a first laser beam and a second laser beam, wherein the predetermined offset frequency shift is relative to a predetermined frequency of either the first laser beam or the second laser beam;

modulating the first laser beam, wherein the modulated first laser beam is to be injected into a device under test (DUT);

acquiring a backscattered signal from the DUT, wherein the backscattered signal results from the modulated first laser beam injected into the DUT, and wherein the second laser beam is to be used as a local oscillator;

determining, based on the acquired backscattered signal from the DUT, a Brillouin trace for the DUT;

repeating the acquisition of the backscattered signal from the DUT for a plurality of frequency shifts;

sampling, based on the repeated acquisitions corresponding to the plurality of frequency shifts and the acquisition of the backscattered signal from the DUT, a distributed Brillouin spectra;

determining, based on the sampling of the distributed Brillouin spectra, a resonant Brillouin frequency shift along the DUT;

scanning the first laser beam and the second laser beam over a wavelength range with a different predetermined offset frequency shift between the two laser beams;

further modulating the first laser beam associated with the different predetermined offset frequency shift, wherein the further modulated first laser beam is to be injected into the DUT;

further acquiring a further backscattered signal from the DUT, wherein the further backscattered signal is based on the further modulated first laser beam injected into the DUT, and wherein the second laser beam is to be used as the local oscillator; and

determining, based on the further acquired backscattered signal from the DUT, a Rayleigh trace for the DUT.

7. The method for Brillouin trace and Rayleigh trace determination according to claim 6 , further comprising:

determining, based on the sampling of the distributed Brillouin spectra, integrated Brillouin power by performing an integration operation with respect to the resonant Brillouin frequency shift.

8. The method for Brillouin trace and Rayleigh trace determination according to claim 7 , wherein the Rayleigh trace represents Rayleigh power versus time or a distance along the DUT, further comprising:

determining, based on the integrated Brillouin power, the Rayleigh power, and the resonant Brillouin frequency shift along the DUT, temperature and strain associated with the DUT.

9. The method for Brillouin trace and Rayleigh trace determination according to claim 6 , wherein the DUT is an optical fiber.

10. The method for Brillouin trace and Rayleigh trace determination according to claim 6 , wherein the predetermined offset frequency shift for determination of the Brillouin trace is approximately 10.8 GHz.

11. The method for Brillouin trace and Rayleigh trace determination according to claim 6 , wherein the predetermined offset frequency shift for determination of the Brillouin trace is selected from a range of approximately 10.0 GHz to approximately 13.0 GHz.

12. A method for Brillouin trace and Rayleigh trace determination, the method comprising:

scanning a first laser beam and a second laser beam over a wavelength range with a predetermined offset frequency shift between the two laser beams, wherein the predetermined offset frequency shift is relative to a predetermined frequency of either the first laser beam or the second laser beam;

modulating the first laser beam, wherein the modulated first laser beam is to be injected into a device under test (DUT);

acquiring a backscattered signal from the DUT, wherein the backscattered signal results from the modulated first laser beam injected into the DUT, and wherein the second laser beam is to be used as a local oscillator;

determining, based on the acquired backscattered signal from the DUT, a Rayleigh trace for the DUT;

maintaining a different predetermined offset frequency shift between the first laser beam and the second laser beam;

further modulating the first laser beam associated with the different predetermined offset frequency shift, wherein the further modulated first laser beam is to be injected into the DUT;

further acquiring a further backscattered signal from the DUT, wherein the further backscattered signal is based on the further modulated first laser beam injected into the DUT, and wherein the second laser beam is to be used as the local oscillator;

determining, based on the further acquired backscattered signal from the DUT, a Brillouin trace for the DUT; and

determining, based on the Brillouin trace, Brillouin power associated with the DUT.

13. The method for Brillouin trace and Rayleigh trace determination according to claim 12 , further comprising:

repeating the acquisition of the backscattered signal from the DUT for the predetermined offset frequency shift; and

averaging, during scanning of the first laser beam and the second laser beam over the wavelength range with the predetermined offset frequency shift between the two laser beams, the repeated acquisitions of the backscattered signal from the DUT for the predetermined offset frequency shift to reduce coherent fading noises.

14. The method for Brillouin trace and Rayleigh trace determination according to claim 12 , wherein the predetermined offset frequency shift is selected from a range of approximately 100.0 KHz to approximately 1.0 GHz.

15. The method for Brillouin trace and Rayleigh trace determination according to claim 12 , wherein the DUT is an optical fiber.

16. The method for Brillouin trace and Rayleigh trace determination according to claim 12 , wherein the Rayleigh trace represents Rayleigh power versus time or a distance along the DUT, further comprising:

normalizing the Brillouin power with respect to the Rayleigh power to remove power variations associated with the DUT; and

determining, based on the normalized Brillouin power and a resonant Brillouin frequency shift along the DUT, temperature and strain associated with the DUT.

Assignments (6)
RELEASE OF SECURITY INTEREST AT REEL/FRAME 73189/0873 Recorded May 28, 2026
From: WELLS FARGO BANK, NATIONAL ASSOCIATION, AS ADMINISTRATIVE AGENT
To: INERTIAL LABS, INC.; VIAVI SOLUTIONS INC.; VIAVI SOLUTIONS LICENSING LLC
Reel/Frame 075642/0381 →
SECURITY INTEREST Recorded Nov 14, 2025
From: VIAVI SOLUTIONS INC.; VIAVI SOLUTIONS LICENSING LLC; INERTIAL LABS, INC.
To: WELLS FARGO BANK, NATIONAL ASSOCIATION, AS AGENT
Reel/Frame 073571/0137 →
SECURITY AGREEMENT Recorded Oct 21, 2025
From: INERTIAL LABS, INC.; VIAVI SOLUTIONS INC.; VIAVI SOLUTIONS LICENSING LLC
To: WELLS FARGO BANK, NATIONAL ASSOCIATION, AS ADMINISTRATIVE AGENT
Reel/Frame 073189/0873 →
TERMINATIONS OF SECURITY INTEREST AT REEL 052729, FRAME 0321 Recorded Jan 5, 2022
From: WELLS FARGO BANK, NATIONAL ASSOCIATION, AS ADMINISTRATIVE AGENT
To: VIAVI SOLUTIONS INC.; RPC PHOTONICS, INC.
Reel/Frame 058666/0639 →
SECURITY INTEREST Recorded May 21, 2020
From: VIAVI SOLUTIONS INC.; 3Z TELECOM, INC.; ACTERNA LLC; ACTERNA WG INTERNATIONAL HOLDINGS LLC; VIAVI SOLUTIONS LLC; JDSU ACTERNA HOLDINGS LLC; OPTICAL COATING LABORATORY, LLC; RPC PHOTONICS, INC.; TTC INTERNATIONAL HOLDINGS, LLC
To: WELLS FARGO BANK, NATIONAL ASSOCIATION, AS ADMINISTRATIVE AGENT
Reel/Frame 052729/0321 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Apr 27, 2016
From: LECOEUCHE, VINCENT
To: VIAVI SOLUTIONS INC.
Reel/Frame 038396/0330 →
Continuity (1)
Related Publication 20170299463A1 · Oct 19, 2017