System and method for gas analysis using doubly resonant photoacoustic spectroscopy

• US 20060123884A1
• Filed: 10/07/2005
• Published: 06/15/2006
• Est. Priority Date: 12/08/2004
• Status: Active Grant

• Current Assignee: Finesse Solutions, Inc. (Thermo Fisher Scientific Incorporated), Li & S Company Limited (Yesco Holdings Co., Ltd.)
• Original Assignee: Skymoon Research & Development Inc.
• Inventors: Paldus, Barbara, Selker, Mark, Riddle, Alfred
• Granted Patent: US 7,263,871 B2
• Time in Patent Office: Days
• US Class Current: 73/24.20
• CPC Class Codes: G01N 2021/1704 in gases
• CPC Class Codes: G01N 21/1702 with opto-acoustic detection, e.g. for gases or analysing solids

Abstract

A method for analyzing gas concentration using doubly resonant photoacoustic spectroscopy, and a doubly resonant photaoacoustic gas detector comprising: i) a continuous wave light beam whose wavelength coincides with an absorption wavelength of a gaseous analyte; ii) a closed path optical cavity having at least two reflective surfaces; iii) an acoustic resonator chamber contained within said optical cavity, and comprising an acoustic sensor for detecting sound waves generated by a gaseous analyte present within said chamber, the light beam passing sequentially into, through and out of said chamber, and being repeatedly reflected back and forth through said chamber, and being modulated at a frequency which is equal to or equal to one-half of an acoustic resonance frequency of said acoustic resonator chamber.

Claims

1. A doubly resonant photaoacoustic gas detector comprising:

i) a continuous wave external light source for generating a light beam whose wavelength coincides with an absorption wavelength of a gaseous analyte;

ii) a closed path optical cavity having at least two reflective surfaces;

iii) an acoustic resonator chamber, said acoustic resonator chamber being contained within said optical cavity, and comprising;

a) an acoustic sensor for detecting sound waves generated by a gaseous analyte present within said chamber,

b) a first entrance port for admitting light from said external light source into said chamber,

c) a second port which passes said light out of said chamber after transmission of said light through said first port and said chamber,

whereby the light beam generated by said external light source passes sequentially into, through and out of said chamber, said light beam being repeatedly reflected back and forth through said chamber, and being modulated at a frequency which is equal to or equal to one-half of an acoustic resonance frequency of said acoustic resonator chamber.

2. The detector of Claim 1 wherein said light beam is modulated at a frequency equal to one-half of an acoustic resonance frequency of said acoustic resonator chamber.

3. The detector of Claim 1 wherein said light beam is modulated at a frequency equal to an acoustic resonance frequency of said acoustic resonator chamber.

4. The detector of Claim 1 wherein said closed path optical cavity comprises at least three reflective surfaces, at least one of said at least three reflective surfaces being translatable.

5. The detector of claim 2 wherein said closed path optical cavity comprises a first reflective surface facing said first port, and a second reflective surface facing said second port, at least one of said first and second reflective surfaces being translatable;

6. The detector of claim 1 wherein the resonance condition of said optical cavity is controlled so as to track the frequency of a wavelength modulatable light beam

7. The detector of claim 1 wherein the external light source is a laser whose frequency is locked by a second, external optical cavity or etalon.

8. A doubly resonant photoacoustic gas detector in accordance with claim 1 wherein said first and second ports comprise optical windows and wherein said at least two reflective surfaces comprise first and second mirrors separate from, but adjacent to, said first and second windows, respectively.

9. A doubly resonant photoacoustic gas detector in accordance with claim 1 wherein said first and second ports are comprised respectively of first and second reflective surfaces.

10. A doubly resonant photoacoustic gas detector in accordance with claim 1 wherein said first port is a Brewster window, a cross-polarizer or a flat antireflection coated window and sais second port comprises a reflective surface.

11. A doubly resonant photoacoustic gas detector in accordance with claim 1 wherein said first and second ports are windowless.

12. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said optical cavity comprises two mirrors

13. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said optical cavity comprises three mirrors

14. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said at least two of said reflective surfaces have a reflectivity of at least 90%.

15. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said acoustic sensor is an electret based microphone, a piezeoelectric based microphone, or a magnetic, balanced armature type microphone.

16. The detector of claim 1 wherein said external light source is a DFB laser, a VCSEL laser, a quantum cascade laser or a fiber laser.

17. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said light source is a diode laser.

18. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said light source is a diode laser emitting light at approximately 1392.53 nm or 1370.96 nm.

19. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said light source is a solid state laser or a CO₂ gas laser.

20. A double resonant photoacoustic gas detector in accordance with claim 6 wherein said light source is a fiber laser

21. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said light source is a quantum cascade laser or an optical parametric oscillator.

22. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said light source and the optical cavity resonant frequency are modulated at substantially the same frequency.

23. A double resonant photoacoustic gas detector in accordance with claim 1 wherein the frequency of said light beam is modulated by translating said translatable reflective surface with a piezoelectric transducer.

24. A double resonant photoacoustic gas detector in accordance with claim 2 wherein said first mirror is translated by a piezoelectric transducer

25. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said acoustic resonator is substantially cylindrical.

26. A double resonant photoacoustic gas detector in accordance with claim 2 wherein said first and second windows are Brewster windows.

27. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said light source is amplitude modulated

28. A double resonant photoacoustic gas detector in accordance with claim 1 wherein said sound waves are modulated at a frequency equal to the second harmonic frequency of said light beam.

29. A double resonant photoacoustic gas detector in accordance with claim 1 wherein at least one mirror is replaced by a crossed polarizer.

30. A method for analyzing gas concentration using doubly resonant photoacoustic spectroscopy, comprising the steps of:

containing a gas sample in an acoustic resonator contained within a resonant external optical cavity;

exciting the gas sample with a beam of excitation light having a wavelength where the gas being analyzed has an absorption feature;

said beam of excitation light being reflected back and forth through said gas sample by at least two reflecting surfaces of said resonant external optical cavity;

oscillating at least one of the reflecting surfaces over a distance such that the external optical cavity tracks the excitation beam'"'"'s full excursion in wavelength space of 1.1 times the full width at half maximum of the absorption feature of said sample gas.