Suppression of stimulated scattering in optical time domain reflectometry

• US 5,592,282 A
• Filed: 07/21/1994
• Issued: 01/07/1997
• Est. Priority Date: 07/22/1993
• Status: Expired due to Term

• Current Assignee: York Limited
• Original Assignee: York Limited
• Inventors: Hartog, Arthur H.
• Primary Examiner(s): McGraw, Vincent P.
• Application Number:
  US08/278,173
• Time in Patent Office: 901 Days
• Field of Search: 250/227.18, 250/227.23, 250/356, 356/43, 356/44, 356/73.1, 356/301, 385/12
• US Class Current: 356/44
• CPC Class Codes: G01K 11/32 using changes in transmittance, scattering or luminescence in optical fibres
• CPC Class Codes: G01M 11/319 Reflectometers using stimulated back-scatter, e.g. Raman or fibre amplifiers

Abstract

Optical time domain reflectometry methods and apparatus are proposed in which the back-scattered optical radiation used to produce output signals is restricted to that resulting from Rayleigh scattering of light launched into a fiber 2 at a first wavelength and that in an anti-Stokes spectral band resulting from Raman or Brillouin scattering of optical radiation at the first wavelength. A first set of output signals produced in dependence upon the anti-Stokes back-scatter may be normalized to the geometric mean of a second set of output signals, produced in dependence upon the Rayleigh back-scatter at the first wavelength, and a third set of output signals, produced in dependence upon Rayleigh back-scatter resulting from light launched into the fiber at the anti-Stokes wavelength. Growth in the intensity of optical radiation in a first Stokes (Raman or Brillouin) spectral band may be inhibited, so as to suppress stimulated scattering, for example by making the fiber 2 high loss at the Stokes wavelength and/or launching into the fiber 2, simultaneously with the pulse at the first wavelength, an additional pulse at a third wavelength equal to that of a Stokes spectral line resulting from inelastic scattering of optical radiation at the first Stokes wavelength. The first wavelength may be chosen so as to minimize the transmission loss, in view of the average losses at the first and detected wavelengths or the increase with wavelength of the launch power which can be used before stimulated scattering has a specified effect.

Claims

1. An optical time domain reflectometry method of sensing respective values of a physical parameter at different locations along an optical fibre, deployed through a region of interest, in which method optical radiation at a first wavelength (λ

₀) is launched into the fibre and back-scattered optical radiation in at least one preselected spectral band is used to produce output signals dependent upon the values being sensed, wherein none of the spectral bands used to produce said output signals lies about a second wavelength (λ

₊₁) which is equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at said first wavelength (λ

₀), is centred, and wherein said first wavelength (λ

₀) and/or said optical fibre are chosen and/or arranged such that relative growth in the intensity in the fibre of optical radiation at said second wavelength (λ

₊₁) is arranged to be inhibited, thereby to suppress conversion in the fibre through stimulated scattering of optical radiation at said first wavelength (λ

₀) to optical radiation at said second wavelength (λ

₊₁).

2. A method as claimed in claim 1, wherein none of the spectral bands used to produce said output signals lies about a further wavelength which is equal to the wavelength on which a further first order Stokes spectral band, which results from another inelastic scattering process in the fibre of optical radiation at said first wavelength (λ

₀), is centred, and relative growth in the intensity in the fibre of optical radiation at said further wavelength is also inhibited, thereby to suppress conversion in the fibre through stimulated scattering of optical radiation at said first wavelength (λ

₀) to optical radiation at said further wavelength.

3. A method as claimed in claim 1, wherein the said one preselected spectral band is an anti-Stokes band resulting from Raman scattering in said fibre.

4. A method as claimed in claim 1, wherein the said one preselected spectral band is an anti-Stokes band resulting from Brillouin scattering in said fibre.

5. A method as claimed in claim 3, wherein back-scattered optical radiation at another preselected spectral band, including said first wavelength (λ

₀), is used in addition to said one preselected spectral band to produce said output signals.

6. A method as claimed in claim 1, wherein said first wavelength (λ

₀) is selected in accordance with a predetermined attenuation characteristic of the fibre such that said first wavelength (λ

₀) and the said one preselected spectral band lie adjacent to a local attenuation coefficient minimum but said second wavelength (λ

₊₁) is displaced from said local attenuation coefficient minimum, optical radiation at said second wavelength (λ

₊₁) thereby being attenuated to a significantly greater extent than optical radiation at said first wavelength (λ

₀) or in the one preselected spectral band.

7. A method as claimed in claim 1, wherein optical radiation at a third wavelength (λ

₂), equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at the said second wavelength (λ

₊₁), is centred, is launched into the fibre simultaneously with said optical radiation at said first wavelength (λ

₀), thereby to cause optical radiation at said second wavelength (λ

₊₁) to be converted to optical radiation at said third wavelength (λ

₊₂) through stimulated scattering, so as to achieve the desired inhibition in growth of optical radiation at said second wavelength (λ

₊₁).

9. A method as claimed in claim 7 or 8, wherein, to inhibit growth in intensity in the fibre of optical radiation at a fourth wavelength (λ

₃), equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at the said third wavelength (λ

₊₂), is centred, optical radiation at a fifth wavelength (λ

₊₄), equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at the said fourth wavelength (λ

₊₃), is centred, is launched into the fibre simultaneously with the optical radiation at said third wavelength (λ

₊₂), thereby to cause optical radiation at said fourth wavelength (λ

₊₃) to be converted to optical radiation at said fifth wavelength (λ

₊₄) through stimulated scattering.

8. An optical time domain reflectometry method of characterising an optical fibre, in which optical radiation at a preset first wavelength (λ

₀) is launched into the fibre and optical radiation back-scattered along the fibre is used to measure a selected characteristic of the fibre, wherein, so as to inhibit growth in the intensity in the fibre of optical radiation at a second wavelength (λ

₊₁), equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at said preset first wavelength (λ

₀), is centred, optical radiation at a third wavelength (λ

₊₂) is launched into the fibre simultaneously with optical radiation at said preset first wavelength (λ

₀), said third wavelength (λ

₊₂) being selected so as to be equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at said second wavelength (λ

₊₁), is centred, thereby causing optical radiation at said second wavelength (λ

₊₁) to be converted to optical radiation at said third wavelength (λ

₊₂) and so suppressing conversion in the fibre of optical radiation at said preset first wavelength (λ

₀) to optical radiation at said second wavelength (λ

₊₁) through stimulated scattering.

10. Optical time domain reflectometry apparatus for sensing respective values of a physical parameter at different locations through a region of interest, which apparatus comprises an optical fibre adapted to be deployed through said region of interest, source means for launching optical radiation at a first wavelength (λ

₀) into the fibre, and detection means for receiving optical radiation back-scattered along the fibre from which respective values of the physical parameter can be derived, wherein filtering means are provided for restricting the back-scattered radiation used to derive said values to one or more preselected spectral bands, none of which lies about a second wavelength (λ

₊₁) which is equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at said first wavelength (λ

₀), is centred, and the said source means and/or the said optical fibre are selected and arranged so as to inhibit growth in the intensity in the fibre of optical radiation at said second wavelength (λ

₊₁), thereby to suppress conversion in the fibre through stimulated scattering of optical radiation at said first wavelength (λ

₀) to optical radiation at said second wavelength (λ

₊₁).

11. Apparatus as claimed in claim 10, wherein the said one preselected spectral band is an anti-Stokes band resulting from Raman scattering in said fibre.

12. Apparatus as claimed in claim 10, wherein the said one preselected spectral band is an anti-Stokes band resulting from Brillouin scattering in said fibre.

13. Apparatus as claimed in claim 11, wherein another preselected spectral band used to produce said output signals lies about said first wavelength (λ

₀).

14. Apparatus as claimed in claim 10, wherein said source means are selected in accordance with a predetermined attenuation characteristic of the fibre such that said first wavelength (λ

₀) and the said one or more spectral bands lie adjacent to a local attenuation coefficient minimum but said second wavelength (λ

₊₁) is displaced from said local attenuation coefficient minimum, optical radiation at said second wavelength (λ

₊₁) thereby being attenuated to a significantly greater extent than optical radiation at said first wavelength (λ

₀) and in the or each spectral band.

15. Apparatus as claimed in claim 14, wherein the said source means are selected such that said second wavelength (λ

₊₁) coincides with an infra-red absorption maximum in the attenuation characteristic of the fibre or lies substantially on the short-wavelength edge of such an absorption maximum.

16. Apparatus as claimed in claim 10, wherein the waveguide structure of the fibre is designed such that loss at the said second wavelength λ

₊₁) is greater than at said first wavelength (λ

₀).

17. Apparatus as claimed in claim 14, wherein said predetermined attenuation characteristic of the fibre has a local absorption maximum corresponding to naturally-occurring, or doped, impurities in the fibre, and said source means are selected such that said second wavelength (λ

₊₁) coincides with said local attenuation maximum or lies substantially on the short-wavelength edge of such an absorption maximum.

18. Apparatus as claimed in claim 17, wherein the said impurities are hydroxide ions.

19. Apparatus as claimed in claim 17, wherein the said impurities are rare earth metal ions.

20. Apparatus as claimed in claim 10, wherein the said optical fibre is provided with built-in gratings for reflecting optical radiation at said second wavelength (λ

₊₁).

21. Apparatus as claimed in claim 10, wherein at least a section of the fibre is bent so as to induce bending loss in the fibre at said second wavelength (λ

₊₁).

22. Apparatus as claimed in claim 10, wherein the said source means are operable to launch optical radiation at a third wavelength (λ

₊₂), equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at the said second wavelength (λ

₊₁), is centred, into the fibre simultaneously with said optical radiation at said first wavelength (λ

₀), thereby to cause optical radiation at said second wavelength (λ

₊₁) to be converted to optical radiation at said third wavelength (λ

₊₂) through stimulated scattering.

23. Apparatus as claimed in claim 22, wherein, to inhibit growth in the intensity in the fibre of optical radiation at a fourth wavelength (λ

₊₃), equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at the said third wavelength (λ

₊₂), is centred, said source means are also operable to launch optical radiation at a fifth wavelength (λ

₊₄), equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at the said fourth wavelength (λ

₊₃), is centred, into the fibre simultaneously with the optical radiation at the said third wavelength (λ

₊₂), thereby to cause optical radiation at said fourth wavelength (λ

₊₃) to be converted to optical radiation at said fifth wavelength (λ

₊₄) through stimulated scattering.

24. Optical time domain reflectometry apparatus for characterising an optical fibre, comprising source means operable to launch optical radiation at a preset first wavelength (λ

₀) into the fibre, and detection means operable to detect optical radiation back-scattered along the fibre which is used to measure a selected characteristic of the fibre, wherein, so as to inhibit growth in the intensity in the fibre of optical radiation at a second wavelength (λ

₊₁), equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at said preset first wavelength (λ

₀), is centred, the source means are also operable to launch optical radiation at a third wavelength (λ

₊₂) into the fibre simultaneously with optical radiation at said preset first wavelength (λ

₀), said third wavelength (λ

₊₂) being equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at said second wavelength (λ

₊₁), is centred, thereby causing optical radiation at said second wavelength (λ

₊₁) to be converted to optical radiation at said third wavelength (λ

₊₂) and so suppressing conversion in the fibre of optical radiation at said preset first wavelength (λ

₀) to optical radiation at said second wavelength (λ

₊₁) through stimulated scattering.

25. An optical time domain reflectometry method for sensing respective values of a physical parameter at different locations along an optical fibre, deployed through a region of interest, in which method optical radiation at a first preselected wavelength (λ

₀) is launched into the fibre and back-scattered optical radiation in at least one preselected spectral band is used to produce output signals dependent upon the values being sensed, wherein none of the spectral bands used to produce said output signals lies about a second wavelength (λ

₊₁) which is equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at said first preselected wavelength (λ

₀), is centered, and said first preselected wavelength (λ

₀) is selected so as to substantially minimise, for a preset length of said fibre, the value of a power loss variable for the fibre concerned, which variable is determined by subtracting from a first wavelength-dependent function, giving the total power loss along the preset length of fibre of forward- and backward-travelling optical radiation, a second wavelength-dependent function giving the maximum forward-travelling power which can be launched into said fibre such that power loss due to stimulated scattering in the fibre does not exceed a predetermined value, both functions being expressed in logarithmic units.

26. Optical time domain reflectometry apparatus for sensing respective values of a physical parameter at different locations through a region of interest, which apparatus comprises an optical fibre adapted to be deployed through said region of interest, source means for launching optical radiation at a first preselected wavelength (λ

₀) into the fibre, detection means for receiving optical radiation back-scattered along the fibre from which respective values of the physical parameter can be derived, and filtering means for restricting the back-scattered radiation used to derive said values to one or more preselected spectral bands, wherein none of the spectral bands used to produce output signals lies about a second wavelength (λ

₊₁) which is equal to the wavelength on which a first order Stokes spectral band, which results from inelastic scattering in the fibre of optical radiation at said first preselected wavelength (λ

₀), is centered, and said first preselected wavelength (λ

₀) is such that, for a preset length of said fibre, the value of a power loss variable for the fibre concerned is substantially minimised, which variable is determined by subtracting from a first wavelength-dependent function, giving the total power loss along the said preset length of fibre of forward- and backward-travelling optical radiation, a second wavelength-dependent function giving the maximum forward-travelling power which can be launched into said fibre such that power loss due to stimulated scattering in the fibre does not exceed a predetermined value, both functions being expressed in logarithmic units.

27. An optical time domain reflectometry method of sensing respective values of a physical parameter at different locations along an optical fibre, deployed through a region of interest, in which method optical radiation at a first wavelength (λ

₀) is launched into the fibre and back-scattered optical radiation in first and second spectral bands, centred respectively on said first wavelength (λ

₀) and a second wavelength (λ

₁) equal to the wavelength of an anti-Stokes spectral band which results from inelastic scattering in the fibre of optical radiation at said first wavelength (λ

₀), is used to produce respective first and second sets of output signals, wherein, non-simultaneously with optical radiation at said first wavelength (λ

₀), optical radiation substantially at said second wavelength (λ

₁) is launched into the fibre and back-scattered optical radiation in a third spectral band, centred on said second wavelength (λ

₁), is used to produce a third set of output signals, and a final set of output signals, dependent upon the values being sensed, is produced by normalising the first set of output signals to the geometric mean of the second and third sets of output signals.

28. Optical time domain reflectometry apparatus for sensing respective values of a physical parameter at different locations through a region of interest, which apparatus comprises an optical fibre adapted to be deployed through said region of interest, source means operable selectively to launch optical radiation at a first wavelength (λ

₀) into the fibre, detection means for receiving optical radiation back-scattered along the fibre, and signal processing means for using such back-scattered optical radiation in first and second spectral bands, centred respectively on said first wavelength (λ

₀) and a second wavelength (λ

₁) equal to the wavelength of an anti-Stokes spectral band which results from an inelastic scattering in the fibre of optical radiation at said first wavelength (λ

₀), to produce respective first and second sets of output signals, wherein said source means are also selectively operable to launch optical radiation substantially at said second wavelength (λ

₁ '"'"') into the fibre, non-simultaneously with optical radiation at said first wavelength (λ

₀), and said signal processing means are operable to use resulting back-scattered optical radiation in a third spectral band, centred on said second wavelength (λ

₁ '"'"'), to produce a third set of output signals, and are further operable to produce a final set of output signals, dependent upon the values being sensed, by normalising the second set of output signals to the geometric mean of the first and third sets of output signals.