Monitoring for disturbance of optical fiber

• US 9,207,168 B2
• Filed: 01/22/2013
• Issued: 12/08/2015
• Est. Priority Date: 01/20/2012
• Status: Active Grant

• Current Assignee: Network Integrity Systems, Inc.
• Original Assignee: Norscan Instruments Ltd.
• Inventors: Lovely, Peter S., Brown, Michael James
• Primary Examiner(s): Toatley, Gregory J
• Assistant Examiner(s): Ayub, Hina F
• Application Number:
  US13/747,326
• Publication Number:
  US 20130188177A1
• Time in Patent Office: 1,050 Days
• Field of Search: 356/73.1, 398 9- 16
• US Class Current: 1/1
• CPC Class Codes: G01M 11/30 Testing of optical devices, constituted by fibre optics or optical waveguides
• CPC Class Codes: G01M 11/33 with a light emitter being disposed at one fibre or waveguide end-face, and a light receiver at the other end-face
• CPC Class Codes: G01M 11/332 using discrete input signals G01M11/333 takes precedence
• CPC Class Codes: G01N 21/21 Polarisation-affecting properties G01N21/19 takes precedence

Abstract

Problems of excessive fading in systems for monitoring single-mode optical fiber for disturbances are addressed by launching into the fiber polarized light having at least two different predetermined launch states of polarization whose respective Stokes vectors are linearly-independent of each other; downstream from the first location, receiving the light from the fiber; analyzing the received light using polarization state analyzer having at least two different analyzer states of polarization that are characterized by respective Stokes vectors that are linearly-independent and detecting the analyzed light to provide corresponding detection signals; deriving from the detection signals measures of changes in polarization transformation properties of the fiber between different times that are invariant under a non-reflective unitary transformation on either the launch states or the detection states; and, on the basis of predefined acceptable physical disturbance criteria determining whether or not the measures are indicative of a reportable physical disturbance.

Claims

1. A method of monitoring an optical fiber, comprising:

launching a probe light flux into the fiber, wherein the probe light flux includes a first portion and a second portion in respective launch polarization states that are characterized by linearly independent launch Stokes vectors;

analyzing a received light associated with propagation of the probe light flux in the fiber based on at least two analyzer polarization states that are characterized by Stokes vectors that are linearly independent;

processing detected signals associated with the analyzed received light to determine a measure of change in the fiber, over a period of time that is substantially invariant under a non-reflecting unitary transformation of either the launch polarization states or the analyzer polarization states; and

reporting a disturbance of the fiber based on the determined measure of change.

2. The method of claim 1, wherein probe light flux portions associated with the each of the two linearly independent launch Stokes vectors are alternately launched into the fiber.

3. The method of claim 2, wherein the probe light flux portions associated with each of the two linearly independent launch Stokes vectors are alternately launched into the fiber in a first time interval and alternately launched in a second time interval, wherein the measure of change is determined based on detected signals associated with the first time interval and the second time interval.

4. The method of claim 1, wherein the probe light flux portions associated with the each of the linearly independent launch Stokes vectors are simultaneously launched into the fiber.

5. The method of claim 4, wherein the probe light flux portions associated with each of the two linearly independent launch Stokes vectors are associated with different wavelengths.

6. The method of claim 5, wherein processing the detected signals further comprises identifying detected signal portions associated with the first portion and the second portion of the probe light flux based on the different wavelengths.

7. The method of claim 4, wherein the probe light flux portions associated with each of the two linearly independent launch Stokes vectors are associated with different modulations.

8. The method of claim 7, wherein processing the detected signals further comprises identifying detected signal portions associated with the first portion and the second portion of the probe light flux based on the different modulations.

9. The method of claim 1, wherein the measure of change is determined based on the detected signals associated with a first time interval and a second time interval.

10. The method of claim 1, wherein the measure of change can be derived from one or more vector representations of Poincaré

sphere rotations corresponding to change or changes during the period of time.

11. The method of claim 1, further comprising:

determining change information over at least two sub-periods that are subsets of the time period;

determining vector representations of Poincaré

sphere rotations corresponding to the change information for the two or more sub-periods; and

determining the measure based partly on relative directional information associated with the two or more vector representations.

12. The method of claim 1, further comprising:

determining change information over at least two sub-periods that are subsets of the time period;

determining vector representations of Poincaré

sphere rotations corresponding to the change information for the two or more sub-periods; and

determining the measure based partly on relative displacement information associated with the two or more vector representations.

13. The method of claim 1, further comprising:

accumulating a set of change information representing a sequence of changes during the period of time; and

computing the measure so as to correspond to components of an isotropic power spectrum that can be represented as a sum of the three power spectra for three components of a corresponding sequence of vector representations of Poincaré

sphere rotations.

14. The method of claim 13, wherein the disturbance is reported based on a power spectrum corresponding to a sum of squares of the three power spectra.

15. The method of claim 14, wherein the disturbance is reported based on a portion of the power spectrum in one or more selected frequency bands.

16. The method of claim 1, wherein the probe light flux further comprises a third portion, wherein the first portion, the second portion, and the third portion are associated with respective linearly independent launch Stokes vectors.

17. The method of claim 1, wherein the received light associated with propagation of the probe light flux in the fiber is analyzed based on at least three analyzer polarization states that are characterized by Stokes vectors that are linearly independent.

18. The method of claim 1, wherein the received light associated with propagation of the probe light flux in the fiber is analyzed based on at least four analyzer polarization states that are characterized by Stokes 4-vectors that are linearly independent.

19. The method of claim 1, wherein the probe light flux is launched into a first end of the fiber and the received light associated with propagation of the probe light flux in the fiber is obtained at a second end of the fiber.

20. An apparatus for monitoring an optical fiber, comprising:

a probe light source coupled to launch a probe light flux into the optical fiber, wherein the probe light flux includes a first portion and a second portion in respective launch polarization states that are characterized by linearly independent launch Stokes vectors;

a polarization analyzer situated to receive a light flux associated with propagation of the probe light flux in the optical fiber and analyze the received light flux based on at least two analyzer polarization states that are characterized by Stokes vectors that are linearly independent; and

a processor configured to receive detected signals associated with the analyzed received light and determine a measure of change in the fiber over a period of time, wherein the measure of change is substantially invariant under a non-reflecting unitary transformation of either the launch polarization states or the analyzer polarization states, wherein the processor is configured to report a disturbance of the optical fiber based on the determined measure of change.

21. The apparatus of claim 20, wherein the probe light source is configured to provide probe light flux portions associated with the each of the two linearly independent launch Stokes vectors and alternately launch the probe light flux portions into the fiber.

22. The apparatus of claim 21, wherein the probe light flux portions associated with each of the two linearly independent launch Stokes vectors are alternately launched into the fiber in a first time interval and alternately launched in a second time interval, wherein the measure of change is determined based on detected signals associated with the first time interval and the second time interval.

23. The apparatus of claim 20, wherein the probe light source is configured to simultaneously launch the probe light flux portions associated with the each of the linearly independent launch Stokes vectors.

24. The apparatus of claim 23, wherein the probe light source is configured so that the probe light flux portions associated with each of the two linearly independent launch Stokes vectors are associated with different wavelengths.

25. The apparatus of claim 24, wherein the processor is configured to process the detected signals so as to identify detected signal portions associated with the first portion and the second portion of the probe light flux based on the different wavelengths.

26. The apparatus of claim 20, wherein the probe light source is configured so that the probe light flux portions associated with each of the two linearly independent launch Stokes vectors are associated with different modulations.

27. The apparatus of claim 26, wherein the processor is configured to identify detected signal portions associated with the first portion and the second portion of the probe light flux based on the different modulations.

28. The apparatus of claim 20, wherein the processor is configured to determine the measure of change based on detected signals associated with a first time interval and a second time interval.

29. The apparatus of claim 20, wherein the measure of change can be derived from a vector representation of Poincaré

sphere rotations corresponding to a change during the period of time.

30. The apparatus of claim 20, wherein the processor is configured to:

determine change information over at least two sub-periods that are subsets of the time period;

determine vector representations of Poincaré

sphere rotations corresponding to the change information for the two or more sub-periods; and

determine the measure based partly on relative directional information or relative displacement information associated with the two or more vector representations.

31. The apparatus of claim 20, wherein the processor determines the measure based on four analyzer polarization states that are characterized by Stokes 4-vectors that are linearly independent.

32. The apparatus of claim 20, wherein the probe light source is configured to produce a periodically varying synchronization light flux, and the processor is configured to establish detected signal portions associated with the first and second portions of the probe light flux based on the periodically varying synchronization light flux.

33. The apparatus of claim 32, wherein the probe light source is configured to provide a third portion, wherein the first portion, the second portion, and the third portion are associated with respective linearly independent launch Stokes vectors.

34. The apparatus of claim 20, wherein the probe light source is coupled to launch the probe light flux into a first end of the optical fiber and the polarization analyzer is situated to receive the light flux associated with propagation of the probe light flux in the optical fiber at a second end of the optical fiber.