Narrow line-width laser characterization based on bi-directional pumped brillouin random fiber laser
US-2015349486-A1 · Dec 3, 2015 · US
US10359302B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10359302-B2 |
| Application number | US-201615380382-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 15, 2016 |
| Priority date | Dec 18, 2015 |
| Publication date | Jul 23, 2019 |
| Grant date | Jul 23, 2019 |
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Using hDVS techniques to detect a disturbance in a coherent Rayleigh backscatter caused by the presence of another optical signal in the fiber. The interaction can be caused by a pump pulse travelling shortly after a probe pulse and at a frequency close to that of the probe plus or minus a Brillouin frequency shift. This results in gain or attenuation of the backscatter signal. The Brillouin shift is a function of temperature and strain.
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The invention claimed is: 1. A system for measuring vibration in a structure, comprising: an optical fiber proximate to the structure having a first end and a second end, wherein a characteristic of the structure causes a backscatter through the optical fiber in response to light being emitted into the optical fiber; a measurement component configured to measure the vibration in the structure as related to the backscatter in the optical fiber, wherein the measurement component is positioned proximate the first end of the optical fiber; a first laser source configured to emit a first laser into the optical fiber proximate the first end of the optical fiber, the first laser having a first frequency; and a second laser source configured to emit a second laser into the optical fiber proximate the first end of the optical fiber, the second laser having a second frequency, wherein a difference between the first frequency and the second frequency is delta-f, wherein delta-f causes an attenuation of a Rayleigh backscatter through a stimulated Brillouin scattering process that causes energy to be transferred from the backscatter to the first laser or the second laser. 2. The system of claim 1 , further comprising one or more acousto-optical modulators on the optical fiber. 3. The system of claim 1 , further comprising one or more fiber amplifiers on the optical fiber. 4. The system of claim 3 wherein the fiber amplifiers are erbium doped fiber amplifiers. 5. The system of claim 1 wherein delta-f is less than a Brillouin shift. 6. The system of claim 5 wherein the first laser interacts with the Rayleigh backscatter generated by the second laser. 7. The system of claim 1 wherein the first laser amplifies the Rayleigh backscatter. 8. The system of claim 7 wherein a gain of at least 5 is achieved. 9. The system of claim 1 wherein the first end of the optical fiber is positioned near a surface of a downhole installation and the second end of the optical fiber is positioned downhole of the first end. 10. The system of claim 1 wherein the characteristic of the structure is at least one of temperature, strain, and vibration. 11. A method of detecting vibration in a structure, the method including: positioning an optical fiber proximate to the structure such that displacement of the structure affects reflective properties of the optical fiber; emitting a probe laser into the optical fiber at a first end of the optical fiber; emitting a pump laser into the optical fiber at the first end, wherein the pump laser and the probe laser have different frequencies separated by a delta-f frequency, and wherein the pump laser is configured to interact with the probe laser to improve a backscatter signal through the optical fiber, wherein the delta-f frequency causes an attenuation of a Rayleigh backscatter through a stimulated Brillouin scattering process that causes energy to be transferred from the backscatter signal to the probe laser or the pump laser. 12. The method of claim 11 , further comprising amplifying one or more of the probe and pump lasers using an erbium doped fiber amplifier. 13. The method of claim 11 , wherein the first end of the optical fiber is toward a surface of a downhole tool, and wherein the second end is further downhole than the first end.
using inelastic backscattering to detect the measured quantity, e.g. using Brillouin or Raman backscattering · CPC title
using elastic backscattering to detect the measured quantity, e.g. using Rayleigh backscattering · CPC title
using fibre optic sensors (light guides per se G02B6/00, acousto-optical devices specially adapted for gating or modulating in optical wave guides G02F1/125) · CPC title
using optical fibres · CPC title
Testing of optical devices, constituted by fibre optics or optical waveguides · CPC title
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