METHOD AND APPARATUS FOR THE PHOTO-ACOUSTIC IDENTIFICATION AND QUANTIFICATION OF ANALYTE SPECIES IN A GASEOUS OR LIQUID MEDIUM

• US 20110214480A1
• Filed: 05/11/2011
• Published: 09/08/2011
• Est. Priority Date: 03/02/2010
• Status: Active Grant

• Current Assignee: Li & S Company Limited (Yesco Holdings Co., Ltd.)
• Original Assignee: Li & S Company Limited (Yesco Holdings Co., Ltd.)
• Inventors: Kachanov, Alexander, Koulikov, Serguei
• Granted Patent: US 8,379,206 B2
• Time in Patent Office: Days
• US Class Current: 73/24.02
• CPC Class Codes: G01N 2021/1704 in gases
• CPC Class Codes: G01N 2021/1708 with piezotransducers probes for investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves G01N29/24
• CPC Class Codes: G01N 21/1702 with opto-acoustic detection, e.g. for gases or analysing solids
• CPC Class Codes: G01N 21/39 using tunable lasers
• CPC Class Codes: H01S 5/005 Optical components external to the laser cavity, specially adapted therefor, e.g. for homogenisation or merging of the beams or for manipulating laser pulses, e.g. pulse shaping H01S5/026, H01S5/18388 take precedence
• CPC Class Codes: H01S 5/0064 Anti-reflection components, e.g. optical isolators
• CPC Class Codes: H01S 5/0656 Seeding, i.e. an additional light input is provided for controlling the laser modes, for example by back-reflecting light from an external optical component H01S5/14, H01S5/4062 and H01S5/4006 take precedence

Abstract

A method and apparatus for the photo-acoustic identification and quantification of one or more analyte species present in a gaseous or liquid medium in low concentration utilizing a laser and a resonant optical cavity containing the medium and having within the cavity at least two partially transparent mirrors, one of which is a cavity coupling mirror and one of which is moveably mounted on an assembly responsive to an input signal.

Claims

1. A method for the identification and quantification of one or more analyte species present in a gaseous or liquid medium utilizing a laser that outputs a laser beam and a resonant optical cavity containing said medium and having at least two cavity mirrors, one of which is a cavity coupling mirror, the method comprising:

coupling the laser beam to the cavity via the cavity coupling mirror using mode matching optics;

applying a periodic dither or modulation waveform to the optical frequency of the laser beam or to the laser itself to thereby induce modulation of the intracavity optical power; and

detecting, at the frequency of the applied dither or modulation waveform or harmonics thereof, a signal representing a varying pressure of the medium within the cavity.

2. The method of claim 1, wherein detecting is performed using a photo-acoustic transducer, and wherein the varying pressure signal is a photo-acoustic signal.

3. The method of claim 1, further including monitoring the intracavity light intensity, using a photodetector located external to the cavity, for use in locking a mean optical frequency of the laser to the frequency of the cavity transmission peak using first or other odd harmonics of the modulation waveform signal.

4. The method of claim 3, further including processing the varying pressure signal at the frequency of the modulation signal or harmonics thereof to produce a normalized pressure signal so as to compensate or correct for variations in the applied modulation waveform and/or variations in the intracavity optical power.

5. The method of claim 4, wherein detecting is performed using a photo-acoustic transducer, and wherein the varying pressure signal is a photo-acoustic signal.

6. The method of claim 1, further including obtaining an electronic waveform proportional to the intracavity optical power by detecting the light intensity emerging from a cavity mirror.

7. The method of claim 6, further including calculating a ratio of a magnitude of the varying pressure signal to a magnitude of the electronic waveform at the detection frequency.

8. The method of claim 1, further including obtaining an absorption spectrum of an analyte by scanning an optical frequency of the cavity resonance peak while maintaining a lock between a mean optical frequency of the laser and the cavity resonance peak.

9. The method of claim 8, wherein scanning the optical frequency of the cavity includes changing an optical length of the cavity.

10. The method of claim 9, wherein at least one of the cavity mirrors is moveable, and wherein changing the optical length of the cavity includes changing a physical length of the cavity by moving a movable cavity mirror.

11. The method of claim 10, further including maintaining a position of the movable cavity mirror within a displacement range, and if the mirror'"'"'s position approaches a displacement range limit, resetting the mirror'"'"'s position to a new position within the displacement range such that a new cavity resonance mode matches a mean optical frequency of the laser.

12. The method of claim 8, wherein maintaining the laser locked to the cavity includes obtaining an error signal and applying the error signal to control the laser mean optical frequency to thereby lock the mean optical frequency of the laser to the cavity resonance peak.

13. The method of claim 8, wherein maintaining the laser locked to the cavity includes obtaining an error signal and applying the error signal to control an optical length of the cavity to thereby lock the cavity resonance peak to the mean optical frequency of the laser.

14. The method of claim 1, further including:

obtaining an error signal; and

locking a cavity resonance peak to a mean optical frequency of the laser using the error signal.

15. The method of claim 1, further including:

obtaining an electronic waveform signal proportional to the intracavity optical power by detecting an intensity of light emerging from a cavity mirror;

calculating a ratio of a magnitude of the varying pressure signal to a magnitude of the electronic waveform signal at the detection frequency; and

simultaneously sampling the varying pressure signal and the electronic waveform signal for use in reducing noise in the varying pressure signal caused by noise in the optical signal of the incident laser beam.

16. The method of claim 15, wherein generation of the dither or modulation waveform is synchronous with sampling of the varying pressure and electronic waveform signals.

17. The method of claim 1, wherein a portion of the light emerging from the cavity coupling mirror reenters a cavity of the laser while maintaining an optical phase that results in periodic optical feedback locking whereby a mean optical frequency of the laser matches a resonance peak of the cavity.

18. The method of claim 17, further comprising:

i) obtaining a time varying photo-detector output signal proportional to the intracavity optical power using a photo-detector located external to the cavity;

ii) obtaining a magnitude of an in-phase component of the time-varying photo-detector output signal at a dither frequency of the dither waveform;

iii) obtaining a magnitude of a quadrature component of the time-varying photo-detector output signal at the dither frequency;

iv) using the in-phase component to maintain a lock between the mean optical frequency of the laser and the resonance peak of the cavity; and

v) increasing or decreasing an optical path difference between the laser and the cavity coupling mirror by inputting to an element adapted to vary the optical path difference between the laser and the cavity coupling mirror a value proportional to the magnitude of the quadrature component of the time varying photo-detector output signal at the dither frequency until the magnitude of the quadrature component zeroes down.

19. The method of claim 1, further including optimizing the amplitude and shape of the applied periodic dither or modulation waveform.

20. The method of claim 19, wherein optimizing includes:

monitoring the intracavity optical power using a photo-detector located external to the cavity; and

repeatedly;

obtaining a magnitude of in-phase and quadrature components of an output signal of the photo-detector at the second harmonic of a dither frequency of the dither waveform;

determining a phase of second harmonic sine and cosine reference functions that zeroes out the quadrature component, and setting a constant phase relative to the phase of the dither waveform to this determined phase; and

determining an optimum laser wavelength dither amplitude that results in a maximum value of the in-phase component of the photo-detector signal at the second harmonic of the dither frequency.

21. The method of claim 20, wherein obtaining the magnitude of the in-phase and quadrature components of the photo-detector output signal includes multiplying the photo-detector output signal by a sine and a cosine reference function having the same frequency as the dither frequency and said constant phase relative to the phase of the dither waveform.