Photoacoustic photon meter and process for measuring photon fluence
US-2020240957-A1 · Jul 30, 2020 · US
US11948548B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11948548-B2 |
| Application number | US-201916969054-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 8, 2019 |
| Priority date | Feb 12, 2018 |
| Publication date | Apr 2, 2024 |
| Grant date | Apr 2, 2024 |
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A phonon parametric oscillator is provided. The phonon parametric oscillator comprises a laser for periodically emitting brief optical pulses (IL), an assembly for generating acoustic pulses (IA) and a medium for coupling the acoustic pulses to an object (O), the assembly for generating acoustic pulses comprising an entrance face, an exit face, a conversion medium for converting the brief optical pulses into acoustic pulses and a propagation medium for propagating said acoustic pulses, the entrance and exit faces being reflective to the acoustic pulses, the propagation medium having a defined thickness, the exit face making contact with the coupling medium. In the phonon parametric oscillator according to the invention, the round-trip time of an acoustic pulse due to reflection from the entrance and exit faces, is equal to the emission period (τ) of the laser, so that the reflected acoustic pulse is in phase with the following acoustic pulse.
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The invention claimed is: 1. A phonon parametric oscillator comprising a laser for periodically emitting brief optical pulses (IL), an assembly for generating acoustic pulses (IA) and a medium for coupling the acoustic pulses to an object (O), the assembly for generating acoustic pulses comprising an entrance face, an exit face, a conversion medium for converting the brief optical pulses into acoustic pulses and a propagation medium for propagating said acoustic pulses, the entrance and exit faces being reflective to the acoustic pulses, the propagation medium having a defined thickness, the exit face making contact with the coupling medium, wherein the round-trip time of an acoustic pulse due to reflection from the entrance and exit faces is equal to the emission period (τ) of the laser, so that the reflected acoustic pulse is in phase with the following acoustic pulse. 2. The phonon parametric oscillator as claimed in claim 1 , wherein the assembly for generating acoustic pulses comprises, in this order, the entrance face, the conversion medium, the propagation medium and the exit face. 3. The phonon parametric oscillator as claimed in claim 1 , wherein the assembly for generating acoustic pulses comprises, in this order, the entrance face, the propagation medium, the conversion medium and the exit face. 4. The phonon parametric oscillator as claimed in claim 1 , wherein the conversion medium and the propagation medium are produced on one and the same substrate, the conversion medium being located on one of the faces of the propagation medium. 5. The phonon parametric oscillator as claimed in claim 1 , wherein the conversion medium and the propagation medium are produced on one and the same substrate, the conversion medium being located inside the propagation medium. 6. The phonon parametric oscillator as claimed in claim 1 , wherein the oscillator comprises means for adjusting the period of the emitting laser. 7. The phonon parametric oscillator as claimed in claim 1 , wherein the oscillator comprises electrical or magnetic or thermal means for adjusting the propagation speed of the acoustic pulses through the propagation medium. 8. The phonon parametric oscillator as claimed in claim 1 , wherein the thickness of the propagation medium varies along an axis perpendicular to the propagation direction of the acoustic pulses. 9. The phonon parametric oscillator as claimed in claim 1 , wherein the acoustic reflection coefficients of the entrance face and of the exit face are higher than or equal to 90%. 10. The phonon parametric oscillator as claimed in claim 1 , wherein the emitting laser is a so-called “femtosecond” laser that emits in a spectral range comprised between 680 nanometers and 1070 nanometers, its period being of 12.5 nanoseconds and the duration of the optical pulses being of 100 femtoseconds. 11. The phonon parametric oscillator as claimed in claim 1 , wherein the emitting laser is a so-called “femtosecond” laser that emits in a spectral range comprised between 750 nanometers and 900 nanometers, its period being of 1 nanosecond and the duration of the optical pulses being of 100 femtoseconds. 12. The phonon parametric oscillator as claimed in claim 1 , wherein the conversion medium is a medium that absorbs the optical pulses. 13. The phonon parametric oscillator as claimed in claim 1 , wherein the conversion medium is a semiconductor medium or one with quantum dots. 14. The phonon parametric oscillator as claimed in claim 1 , wherein the propagation medium is silicon or diamond or silicon carbide or sapphire. 15. The phonon parametric oscillator as claimed claim 1 , wherein the coupling medium is a liquid.
using optical excitation, e.g. laser bundle · 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
providing acoustic coupling {, e.g. water (impedance matching G10K11/02)} · CPC title
with frequency characteristics, e.g. single frequency signals, chirp signals (measuring frequency of mechanical vibrations or acoustic waves in general G01H1/06, G01H3/04; measuring frequency or analysing frequency spectra G01R23/00) · CPC title
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