Optical fiber temperature distribution measuring device
US-9835503-B2 · Dec 5, 2017 · US
US12130189B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-12130189-B2 |
| Application number | US-202117191622-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 3, 2021 |
| Priority date | Apr 13, 2020 |
| Publication date | Oct 29, 2024 |
| Grant date | Oct 29, 2024 |
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Aspects of the present disclosure describe distributed fiber optic sensing systems (DFOSa), methods, and structures for distributed temperature sensing (DTS) that 1) employs a GmAPD instead of a traditional LmAPD detector which advantageously produces a 10˜20 dB gain improvement of SNR for a far-end weak signal, thereby improving long range detectability; 2) employs an inventive gating scheme that advantageously and surprisingly overcomes the “dead time” problem for GmAPD working in SPC mode that plagues Geiger mode operation; and 3) third, employs an inventive post-processing technique that advantageously allows our methods to correct any dark noise caused signal distortion.
Opening claim text (preview).
The invention claimed is: 1. A distributed fiber optic sensing (DFOS) system for distributed temperature sensing (DTS) comprising: the DTS system configured to measure the temperature along a length of optical fiber by providing laser light pulse(s) to the optical fiber and detecting Raman-based backscattered light, said backscattered light including temperature information in its intensity; the DFOS system including a Geiger-mode avalanche photo detector (GmAPD) configured to operate in a single photon counting (SPC) mode, and a gating signal applied to the GmAPD such that a sensitivity of the GmAPD is limited in a high-intensity light condition; the DFOS system CHARACTERIZED BY: a gating signal applied to an output signal of the GmAPD, wherein such gating signal is inversely proportional to a detected light intensity such that the higher the detected light intensity the less sensitive the detection. 2. The system of claim 1 further CHARACTERIZED BY: the rate of the gating signal is lower than an actual photon rate associated with a near-end of the optical fiber and higher than an actual photon rate associated with a far-end of the optical fiber. 3. The system of claim 2 further CHARACTERIZED BY: a dark noise correction applied to the output signal of the GmAPD.
Raman spectrometry; Scattering spectrometry {; Fluorescence spectrometry} · CPC title
using Raman scattering · CPC title
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