IP Library Granted Patent US 10,101,182
Granted Patent B2
US 10,101,182 · App. 15/116,500 · Granted Oct 16, 2018

Interferometric high fidelity optical phase demodulation using 120 degree phase separation

Inventor: David A. Barfoot (Houston, TX)
Assignee: HALLIBURTON ENERGY SERVICES, INC.
G01D5/35306E21B47/06E21B47/065E21B47/123E21B47/14G01J9/02G01J2009/0226
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Quick Facts
Patent No.
US 10,101,182
App. No.
15/116,500
Granted
Oct 16, 2018
Kind
B2
Abstract

An illustrative interferometric system with high-fidelity optical phase demodulation includes a receiver having a fiberoptic coupler that produces optical interferometry signals having mutual phase separations of 120° and balanced photo-detectors that each produce an electrical difference signal based on a respective pair of said optical interferometry signals. The system further includes circuitry that converts the electrical difference signals into measurements of an interferometric phase.

Claims (47)

1. An interferometric system with high-fidelity optical phase demodulation, comprising:

a receiver having:

a fiberoptic coupler that produces optical interferometry signals having mutual phase separations of 120°;

balanced photo-detectors that each produce an electrical difference signal based on a respective pair of said optical interferometry signals;

circuitry that converts the electrical difference signals into measurements of an interferometric phase; and

a source that transmits at least one light pulse along a distributed sensing fiber, wherein the circuitry windows said measurements based on a time delay after each pulse to associate said measurements with a position on the distributed sensing fiber.

2. The system of claim 1 , wherein the distributed sensing fiber couples one or more return signals to the receiver, and wherein the receiver splits the one or more return signals across two optical paths having a propagation delay difference to enable the fiberoptic coupler to produce said optical interferometry signals.

3. The system of claim 2 , further comprising a first circulator that couples said at least one light pulse from the source to the distributed sensing fiber, and further couples at least one of the one or more return signals to the receiver.

4. The system of claim 2 , wherein the fiberoptic coupler splits at least one of the one or more return signals across the two optical paths, and wherein the two optical paths are reflectively terminated.

5. The system of claim 4 , wherein said optical paths are reflectively terminated with faraday rotator mirrors.

6. The system of claim 4 , wherein the receiver further comprises a second circulator that couples the one or more return signals to the fiberoptic coupler, and that further couples one of said optical interferometry signals to at least one of the balanced photo-detectors.

7. The system of claim 1 , wherein the receiver further comprises one or more splitters that each distribute one of the optical interferometry signals to two of said balanced photo-detectors.

8. The system of claim 7 , wherein the optical interferometry signals comprise three optical interferometry signals, and wherein the balanced photo-detectors comprise three balanced photo-detectors that each produce an electrical difference signal between every pair of said three optical interferometry signals.

9. The system of claim 7 , further comprising:

a circulator that couples said at least one light pulse from the source to the distributed sensing fiber, and further couples a return signal to the receiver;

an optical frequency shifter that couples the source to the fiberoptic coupler;

a local oscillator which generates a local oscillator output signal; and

one or more frequency mixers, each mixer configured to receive the local oscillator output signal and the electrical difference signals from one of the balanced photo-detectors, and thereby generate a mixer output signal.

10. The system of claim 9 , wherein the optical frequency shifter is an acousto-optic modulator.

11. The system of claim 9 , wherein the optical frequency shifter comprises an optical phase shifter driven by a sawtooth or linear ramp function.

12. The system of claim 9 , further comprising one or more low-pass filters, each low-pass filter coupled to one of the one or more frequency mixers and configured to generate a filtered output signal.

13. The system of claim 1 , wherein the circuitry comprises:

at least one analog to digital converter that digitizes said electrical difference signals; and

a processing unit that combines digitized electrical difference signals to obtain an interferometric phase signal.

14. A method of measuring interferometric phase with high-fidelity optical phase demodulation, comprising:

transmitting at least one light pulse along a distributed sensing fiber with a source;

producing optical interferometry signals having mutual phase separations of 120° with a fiberoptic coupler;

performing balanced detection on each of multiple pairs of said optical interferometry signals to obtain corresponding electrical difference signals;

converting the electrical difference signals into measurements of an interferometric phase with circuitry, each of said measurements being associated with a corresponding position along the distributed sensing fiber; and

windowing said measurements with the circuitry based on a time delay after each pulse to associate said measurements with a position on the distributed sensing fiber.

15. The method of claim 14 , wherein the distributed sensing fiber couples one or more return signals to a receiver, the method further comprising splitting the one or more return signals across two optical paths with the receiver, wherein the two optical paths have a propagation delay difference to enable the fiberoptic coupler to produce said optical interferometry signals.

16. The method of claim 15 , wherein the fiberoptic coupler splits the one or more return signals across the two optical paths, and wherein the two optical paths are reflectively terminated.

17. The method of claim 16 , wherein said optical paths are reflectively terminated with faraday rotator mirrors.

18. The method of claim 14 , further comprising splitting the optical interferometry signals with one or more splitters that each distributes one of the optical interferometry signals to two balanced photo-detectors.

19. The method of claim 18 , further comprising:

generating a local oscillator output signal with a local oscillator;

generating a frequency shifted signal with an optical frequency shifter which receives a signal from the source and the local oscillator output signal;

receiving the shifted signal with a fiberoptic coupler; and

receiving the local oscillator output signal and the electrical difference signals from one of the two balanced photo-detectors with one or more frequency mixers, each of the one or more frequency mixers generating a mixer output signal.

20. The method of claim 19 , wherein the optical frequency shifter is an acousto-optic modulator.

21. The method of claim 19 , wherein the optical frequency shifter comprises an optical phase shifter driven by a sawtooth or linear ramp function.

22. The method of claim 19 , further comprising:

filtering the mixer output signal with one or more low-pass filters; and

generating a filtered output signal from each of the one or more low-pass filters.

23. The method of claim 14 , wherein the circuitry further comprises:

digitizing said electrical difference signals with at least one analog to digital converter; and

processing the digitized electrical difference signals with a processing unit to obtain an interferometric phase signal.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 3, 2016
From: BARFOOT, DAVID A.
To: HALLIBURTON ENERGY SERVICES, INC.
Reel/Frame 039336/0108 →
Continuity (1)
Related Publication 20170010133A1 · Jan 12, 2017
Cited By (3)
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