Computing emission rate from gas density images
US-2024420311-A1 · Dec 19, 2024 · US
US9784673B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9784673-B2 |
| Application number | US-201514842589-A |
| Country | US |
| Kind code | B2 |
| Filing date | Sep 1, 2015 |
| Priority date | Oct 16, 2014 |
| Publication date | Oct 10, 2017 |
| Grant date | Oct 10, 2017 |
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A method and system for optical angular momentum (OAM) spectroscopy includes generating a beam of light having a single OAM mode. A first spectrum of the beam of light is detected and the beam of light is passed through a gas to attenuate the beam of light in accordance with a presence and concentration of a respective gas. A second spectrum the beam of light is coherently detected and a difference between the first and second spectrum for the beam of light is analyzed to determine the presence and concentration of the respective gas.
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The invention claimed is: 1. A method for optical angular momentum (OAM) spectroscopy, comprising: generating a plurality of beams of light, each beam having a different respective OAM mode, by splitting a laser beam and imposing a respective OAM mode onto each of the split beams; detecting a first absorption spectrum of each of the beams of light; passing the beams of light through a gas at the same time to attenuate the beams of light in accordance with a presence and concentration of a respective gas after detecting the first absorption spectra; coherently detecting a second absorption spectrum of each of the beams of light; and analyzing a difference between the first and second absorption spectra for the beams of light to determine the presence and concentration of the respective gas. 2. The method of claim 1 , wherein the laser beam has a wavelength in the middle infrared range. 3. The method of claim 1 , wherein imposing an OAM mode on a beam of light comprises passing the beam through a phase plate. 4. The method of claim 1 , wherein imposing an OAM mode on a beam of light comprises passing the beam through a hologram plate. 5. The method of claim 1 , wherein analyzing the difference between the first and second spectrum comprises matching the difference to an expected spectrum for the respective gas. 6. The method of claim 1 , further comprising splitting the beam of light into orthogonal polarizations before the beam passes through the gas. 7. The method of claim 6 , wherein coherently detecting the second spectrum comprises independently detecting each of the orthogonal polarizations. 8. An optical angular momentum (OAM) spectroscopy sensor, comprising: a laser configured to output a plurality of unconverted beams; an OAM converter configured to impose a respective OAM mode on each of the unconverted beams to produce respective OAM beams; a first OAM receiver configured to detect a first absorption spectrum of each of the OAM beams from the OAM converter; a gas cavity containing a mixture comprising one or more component gases configured to attenuate each of the OAM beams at the same time in accordance with a presence and concentration of a respective gas; a second OAM receiver configured to coherently detect a second absorption spectrum of each of the OAM beams after the OAM beams have passed through the gas cavity; and a processor configured to analyze a difference between the first and second absorption spectra for the beams of light to determine the presence and concentration of the respective gas. 9. The sensor of claim 8 , wherein the laser output has a wavelength in the middle infrared range. 10. The sensor of claim 8 , wherein the OAM converter comprises a phase plate to impose an OAM mode on a beam. 11. The sensor of claim 8 , wherein the OAM converter comprises a hologram plate to impose an OAM mode on a beam. 12. The sensor of claim 8 , wherein the processor is further configured to match the difference to an expected spectrum for the respective gas. 13. The sensor of claim 8 , further comprising a polarizing splitter configured to split the OAM beam into orthogonal polarizations before the beam passes through the gas cavity. 14. The sensor of claim 13 , wherein the second OAM receiver is configured to independently detect each of the orthogonal polarizations.
using photo-electric detection (G01N21/31 takes precedence){; circuits for computing concentration (logarithmic circuits G06G7/24; photometric circuits in general G01J)} · CPC title
Coherent sources; lasers · CPC title
for analysing gases, e.g. multi-gas analysis · CPC title
Polarisation-affecting properties (G01N21/19 takes precedence) · CPC title
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