Optical time domain reflectometry for two segment fiber optic systems having an optical amplifier therebetween
An optical time domain reflectometry apparatus for sensing a parameter in a region of interest is characterized in that the optical fiber includes a first section into which optical radiation at the probe wavelength is launched and a second section deployed in the region of interest. The first section has a higher intensity threshold for the onset of non-linear effects than the second section. The source launches the optical radiation into the first section at an intensity lower than the non-linear effects intensity threshold of the first section but higher than the non-linear effects intensity threshold of the second section. The attenuation characteristics of the first section are chosen such that the intensity of the optical radiation at the probe wavelength that reaches the second section is below the threshold for the onset of non-linear effects of the second section.
1. An optical time domain reflectometry apparatus, for sensing a parameter to be measured in a region of interest, the apparatus comprising:
an optical fiber;
a source operable to launch optical radiation into the optical fiber at a probe wavelength having a preselected intensity, wherein the optical fiber includes a first section, into which the optical radiation at the probe wavelength is launched, and a second section deployed in the region of interest;
detection means operable to produce electrical output signals in response to optical radiation backscattered from the optical fiber; and
a remote amplifier arranged between the first and second sections which is operable to compensate for attenuation losses in the intensity of the probe wavelength in the first section, wherein the remote amplifier comprises a section of fiber doped with rare-earth ions, the fiber exhibiting gain at the probe wavelength when illuminated by the optical radiation at a pump wavelength and wherein the gain of the remote amplifier is selected to increase the intensity of the optical radiation transmitted into the second section to a value just below an intensity threshold for the onset of non-linear effects of the second section, thereby allowing the intensity of the radiation launched into the first section to be low compared to the intensity threshold for the onset of non-linear effects of the first section.
2. The apparatus of claim 1 , wherein the remote amplifier comprises a single mode fiber doped with erbium ions.
3. The apparatus of claim 1 , further comprising a wavelength-selective reflector provided at a remote end of the remote amplifier for reflecting any unabsorbed optical radiation at the pump wavelength back through the remote amplifier.
4. Apparatus as claimed in claim 3 , wherein the reflector preferably comprises a fiber Bragg grating.
5. The apparatus of claim 1 , wherein the remote amplifier forms part of an optical sub-assembly provided between the first and second sections, the sub-assembly operable to separate the optical radiation at the probe wavelength from the backscattered optical radiation and transmit it, via the remote amplifier and filtering means for filtering out optical radiation at unwanted wavelengths, into the second section.
6. The apparatus of claim 5 , wherein the optical sub-assembly further includes a second amplifier for amplifying backscattered optical radiation returned from the second section.
7. The apparatus of claim 5 , wherein the optical sub-assembly further comprises a first and a second input/output circulator optically connected to the first and second sections respectively.
8. The apparatus of claim 7 , wherein the first input/output circulator is connected to the first section by a directional coupler, the directional coupler arranged to transmit optical radiation at the pump wavelength to the remote amplifier.
9. The apparatus of claim 5 , wherein a length of the second section of the optical fiber is less than or equal to a length of the first section of the optical fiber.
10. The apparatus of claim 1 , wherein the first section comprises a first and a second fiber, the first fiber being arranged so as to convey the optical radiation at the probe wavelength toward the second section and the second fiber being arranged to convey the backscattered optical radiation returned from the second section to the detecting means.
11. The apparatus of claim 10 , wherein the optical radiation at the pump wavelength is also launched into the first fiber of the first section.
12. The apparatus of claim 1 , wherein a length of the second section of the optical fiber is less than or equal to a length of the first section of the optical fiber.
13. An optical time domain reflectometry apparatus, for sensing a parameter to be measured in a region of interest, the apparatus comprising:
an optical fiber;
a source operable to launch optical radiation into the optical fiber at a probe wavelength having a preselected intensity, wherein the optical fiber includes a first section, into which the optical radiation at the probe wavelength is launched, and a second section deployed in the region of interest;
detection means operable to produce electrical output signals in response to optical radiation backscattered from the optical fiber; and
a remote amplifier arranged between the first and second sections which is operable to compensate for attenuation losses in the intensity of the probe wavelength in the first section, wherein the remote amplifier comprises a section of fiber doped with rare-earth ions, the fiber exhibiting gain at the probe wavelength when illuminated by the optical radiation at a pump wavelength and wherein the remote amplifier forms part of an optical sub-assembly provided between the first and second sections, the sub-assembly operable to separate the optical radiation at the probe wavelength from the backscattered optical radiation and transmit it, via the remote amplifier and filtering means for filtering out optical radiation at unwanted wavelengths, into the second section.
14. The apparatus of claim 13 , wherein the remote amplifier comprises a single mode fiber doped with erbium ions.
15. The apparatus of claim 13 , further comprising a wavelength-selective reflector provided at a remote end of the remote amplifier for reflecting any unabsorbed optical radiation at the pump wavelength back through the remote amplifier.
16. Apparatus as claimed in claim 15 , wherein the reflector preferably comprises a fiber Bragg grating.
17. The apparatus of claim 13 , wherein the gain of the remote amplifier is selected to increase the intensity of the optical radiation transmitted into the second section to a value just below an intensity threshold for the onset of non-linear effects of the second section, thereby allowing the intensity of the radiation launched into the first section to be low compared to the intensity threshold for the onset of non-linear effects of the first section.
18. The apparatus of claim 13 , wherein the optical sub-assembly further includes a second amplifier for amplifying backscattered optical radiation returned from the second section.
19. The apparatus of claim 13 , wherein the optical sub-assembly further comprises a first and a second input/output circulator optically connected to the first and second sections respectively.
20. The apparatus of claim 19 , wherein the first input/output circulator is connected to the first section by a directional coupler, the directional coupler arranged to transmit optical radiation at the pump wavelength to the remote amplifier.
21. The apparatus of claim 13 , wherein the first section comprises a first and a second fiber, the first fiber being arranged so as to convey the optical radiation at the probe wavelength toward the second section and the second fiber being arranged to convey the backscattered optical radiation returned from the second section to the detecting means.
22. The apparatus of claim 21 , wherein the optical radiation at the pump wavelength is also launched into the first fiber of the first section.
23. The apparatus of claim 13 , wherein a length of the second section of the optical fiber is less than or equal to a length of the first section of the optical fiber.