Compact near-IR and mid-IR cavity ring down spectroscopy device

• US 7,541,586 B2
• Filed: 11/10/2006
• Issued: 06/02/2009
• Est. Priority Date: 11/10/2006
• Status: Expired due to Fees

• Current Assignee: George Washington University
• Original Assignee: George Washington University
• Inventors: Miller, J. Houston
• Primary Examiner(s): Porta; David P
• Assistant Examiner(s): Green; Yara B
• Application Number:
  US11/558,445
• Publication Number:
  US 20080111077A1
• Time in Patent Office: 935 Days
• Field of Search: None
• US Class Current: 250/339.07
• CPC Class Codes: G01N 2021/399 Diode laser
• CPC Class Codes: G01N 21/3504 for analysing gases, e.g. multi-gas analysis
• CPC Class Codes: G01N 21/359 using near infrared light
• CPC Class Codes: G01N 21/39 using tunable lasers

Abstract

This invention relates to a compact cavity ring down spectrometer for detection and measurement of trace species in a sample gas using a tunable solid-state continuous-wave mid-infrared PPLN OPO laser or a tunable low-power solid-state continuous wave near-infrared diode laser with an algorithm for reducing the periodic noise in the voltage decay signal which subjects the data to cluster analysis or by averaging of the interquartile range of the data.

Claims

1. A compact cavity ring down spectroscopy apparatus for detection and measurement of trace species in a sample gas, which comprises:

a housing for said apparatus;

a tunable solid-state continuous-wave mid-infrared PPLN OPO laser within said housing;

an acousto-optic modulator in fiber optical communication with said laser for steering a first order diffraction beam of said laser and for interrupting said beam when resonance is achieved;

a ring down resonant cavity within the housing for holding a sample gas, said cavity cell receiving said first order diffraction beam of said laser and comprising at least two high-reflectivity mirrors, wherein said mirrors define an intracavity light path and one of said mirrors is a movable tuning mirror, wherein the cavity has 4 mirrors in a bowtie configuration;

a piezo transducer drive attached to the tuning mirror for modulating cavity length to maintain resonance between the laser frequency and cavity modes; and

a photo-detector within said housing, for receiving said beam from the cavity and for generating a resonance signal and a voltage decay (ring down) signal, thereby measuring an interaction of said sample with said intracavity beam; and

,

a microprocessor for reducing the periodic noise in the voltage decay signal by recording the cw-CRD voltage decay signals as data and subjecting the data to a cluster analysis or averaging the interquartile range of the data;

wherein the trace species of the sample gas is selected from the group consisting of;

HCHO, H2S, methyl mercaptan, CO2, CO, HCN, HCl, NH3, C2H2, sarin, VX, mustard gas, arsine, phosgene, tear gas, pepper gas, nitro-based explosive, and B2; and

,

wherein the apparatus is configured as a desktop apparatus wherein the foot print is between about 6″

to about 12″

wide, by about 5″

to about 8″

deep, by about 5″

to about 8″

tall.

2. The apparatus of claim 1, configured as a desktop apparatus wherein the foot print is between about 8.5″

wide, by about 6.5″

deep, by about 4″

tall.

3. The apparatus of claim 1, configured to weigh about 5 pounds to about 12 pounds.

4. The apparatus of claim 1, configured to weigh about 6 pounds.

5. The apparatus of claim 1, configured to fit in a 2U box for standard 19″

rack.

6. A method for determining an exponential decay rate of a signal in a cavity ring down spectroscopic analysis, said method comprising:

providing the apparatus of claim 1 a ring down resonant cavity for holding a sample gas, wherein the cavity has at least one tunable mirror;

illuminating the cavity with said tunable solid-state continuous-wave mid-infrared PPLN OPO laser;

matching the cavity length to the laser frequency by moving the tunable mirror until resonance is detected;

interrupting the laser beam; and

detecting one or more decay signals.

7. The method of claim 6, wherein the tunable mirror comprises a high reflectivity mirror attached to a piezo transducer driver.

8. The method of claim 6, wherein interrupting the laser beam comprises switching off an acousto-optic modulator.

9. The method of claim 6, wherein the decay signals generated during resonance number between about 1 kHz to about 20 kHz.

10. The method of claim 6, wherein the decay signals generated during resonance number between about 10 kHz to about 20 kHz.

11. The method of claim 6, further comprising the step of:

maintaining resonance within the cavity by switching the AOM back on and monitoring the cavity for resonance, wherein decay signals continue to be detected if resonance is detected within the cavity, and wherein cavity modulation by moving the tunable mirror is performed if resonance is not detected within the cavity.

12. The method of claim 6, further comprising the steps of:

recording the decay signals as data; and

and subjecting the data to a cluster analysis to reduce the periodic noise in cw-CRD spectra when using cavity modulation.

13. The method of claim 6, further comprising the steps of:

recording the decay signals as data; and

averaging the interquartile range, wherein discarding the upper and lower quartiles before averaging the data values reduces the periodic noise in cw-CRD spectra when using cavity modulation.