Photoabsorption remote sensing (pars) imaging methods
US-2024255427-A1 · Aug 1, 2024 · US
US9995674B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9995674-B2 |
| Application number | US-201414584004-A |
| Country | US |
| Kind code | B2 |
| Filing date | Dec 29, 2014 |
| Priority date | Dec 26, 2013 |
| Publication date | Jun 12, 2018 |
| Grant date | Jun 12, 2018 |
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A laser vibrometer for measurement of ambient chemical species includes a laser that produces a beam that is split into a reference readout beam and a signal readout beam. A probe laser beam is tuned to an absorption feature of a molecular transition, and generates acoustic signals when incident on a gaseous species via the photo acoustic effect. The scattered acoustic signals are incident on a thin membrane that vibrates. The readout laser beam reflected from the vibrating membrane is mixed with the reference beam at the surface of a photo-EMF detector. Interferrometric fringes are generated at the surface of the photo-EMF detector. Electric current is generated in the photo-EMF detector when the fringes are in motion due to undulations in the signal readout beam imparted by the vibrating membrane. A highly sensitive photo-EMF detector is capable of detecting picoJoules or less laser energy generated by vibrating processes.
Opening claim text (preview).
What is claimed is: 1. A laser vibrometer capable of detecting chemical species, comprising: a light source configured to produce beams of monochromatic light including: an external probe beam, having a wavelength corresponding to an absorption feature of the chemical species to be detected; a reference beam; and a sensing beam; a pressure-sensing diaphragm which when impacted by the pressure waves resulting from the external probe beam interacting with a chemical species that is located away from the sensing beam responsively vibrates; a photo-electromotive force (photo-EMF) sensor; wherein the sensing beam is directed against the second side of the pressure sensing diaphragm; and wherein the sensing beam is directed to the photo-EMF sensor from the pressure-sensing diaphragm which photo-EMF sensor outputs a signal corresponding to the displacement of the diaphragm caused by the incident pressure wave. 2. The laser vibrometer of claim 1 , wherein the light source includes: a laser configured to produce a beam of monochromatic light having a wavelength corresponding to an absorption feature of the chemical species to be detected; a first beam splitter configured to split the beam of monochromatic light into the external probe beam and an internal beam; and a second beam splitter configured to split the internal beam into the reference beam and the sensing beam, the reference beam being directed to a photosensor. 3. The laser vibrometer of claim 2 , including: an external mirror configured to reflect the external probe beam. 4. The laser vibrometer of claim 3 , including: a lens configured to direct the external probe beam after the external probe beam reflects from the external mirror. 5. The laser vibrometer of claim 1 , wherein the laser produces a beam of light having a wavelength of about 2.3 microns to detect carbon monoxide. 6. The laser vibrometer of claim 1 , wherein: the laser produces a beam of light having a wavelength of 1.6 or 3.3 microns to detect methane. 7. The laser vibrometer of claim 1 , wherein: the laser comprises a nonlinear device configured to generate tunable laser wavelengths. 8. The laser vibrometer of claim 1 , including: a housing defining an interior space, and wherein the light source, the pressure-sensing diaphragm, and the photo-EMF sensor are disposed in the interior space. 9. The laser vibrometer of claim 8 , wherein: the external probe beam travels outside of the housing. 10. The laser vibrometer of claim 1 , wherein: the pressure-sensing diaphragm comprises ZnO that is nanolayered onto a silicon-based layer of material. 11. The laser vibrometer of claim 10 , wherein: the silicon-based layer of material comprises a silicon carbide. 12. The laser vibrometer of claim 1 , wherein: the photo-EMF sensor comprises detector material defining a bandgap that is tuned based on the absorption features of a chemical species that is to be detected. 13. The laser vibrometer of claim 12 , wherein: the detector material comprises CdSe having multiple doping of transition elements into the CdSe. 14. The laser vibrometer of claim 12 , wherein: the photo-EMF sensor comprises a nanotechnology based bandgap tuned device. 15. The laser vibrometer of claim 12 , wherein: Wherein the reference beam is shifted to a different frequency than that of the sensing beam. 16. A chemical species detector, comprising: a light source configured to produce beams of monochromatic light including: a first beam, having a wavelength corresponding to an absorption feature of the chemical species to be detected; a second beam; and a third beam; a pressure-sensing diaphragm which when impacted by the pressure waves resulting from the first beam interacting with a chemical species that is located away from the third beam responsively vibrates; a photo-electromotive force (photo-EMF) sensor, configured and arranged to detect displacements of the pressure sensing diaphragm as little as 10 femtometers; a housing defining an interior space, and wherein the light source the pressure-sensing diaphragm, the photo-EMF sensor, the second beam and the third beam are contained within the interior space; wherein the chemical species is located outside of the interior space and the first beam is directed outside of the interior space; wherein the third beam is directed against the second side of the pressure sensing diaphragm; and wherein the third beam is directed to the photo-EMF sensor from the pressure-sensing diaphragm which photo-EMF sensor outputs a signal corresponding to the displacement of the diaphragm caused by the incident pressure wave; and wherein the second beam is frequency shifted from that of the third beam and the sensor is configured to perform phase measurements by heterodyning a frequency shifted second beam and the third beam.
in gases · CPC title
by spectral analysis, e.g. Fourier analysis {or wavelet analysis (spectral signal processing per se G06F17/14)} · CPC title
using optoacoustic interaction with the material, e.g. laser radiation, photoacoustics (photoacoustic cells G01N21/1702; measuring characteristics of vibrations by using radiation-sensitive means G01H9/00; acousto-optical conversion techniques for short-range imaging G01S15/8965; sound-producing devices using laser bundle G10K15/046) · CPC title
the vibrations causing a variation in the relative position of the end of a fibre and another element · CPC title
with opto-acoustic detection, e.g. for gases or analysing solids · CPC title
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