Dual beam acousto-optic tunable spectrometer

• US 5,039,855 A
• Filed: 03/05/1990
• Issued: 08/13/1991
• Est. Priority Date: 03/05/1990
• Status: Expired due to Term

• Current Assignee: BRAN & Luebbe Incorporated
• Original Assignee: Bran+Luebbe Analyzing Technologies Incorporated
• Inventors: Evans, James, Kemeny, Gabor J., Rachlis, Robert E., Ashraf, Aamir, Soryn, Carl G., Mark, Howard
• Primary Examiner(s): Fields, Carolyn E.
• Assistant Examiner(s): Dunn, Drew A.
• Application Number:
  US07/488,687
• Time in Patent Office: 526 Days
• Field of Search: 250/345, 250/343, 250/339, 356/436, 356/437, 350/358, 350/370
• US Class Current: 250/339.07
• CPC Class Codes: G01J 3/1256 using acousto-optic tunable filter; acousto-optic elements or systems G02F1/11, G02F1/33
• CPC Class Codes: G01J 3/42 Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry beam switching arrangements G01J3/08
• CPC Class Codes: G01N 2021/0346 Capillary cells; Microcells
• CPC Class Codes: G01N 21/0332 with temperature control control of temperature G05D23/00; cryostats F17C3/08
• CPC Class Codes: G01N 21/05 Flow-through cuvettes G01N21/09 takes precedence; handling fluid samples G01N1/10
• CPC Class Codes: G01N 2201/0638 Refractive parts
• CPC Class Codes: G01N 2201/08 Optical fibres; light guides

Abstract

A dual beam acousto-optic tunable spectrometer utilizes an optics system to isolate the two radiation beams tuned by an acousto-optic filter, one of which is used to analyze a sample, the other of which is used as a reference. The tuning of the filter and the analysis of the signals is conducted by a microprocessor, which corrects for the many possible sources of noise. A new fluid sample cell utilizing glass balls to collimate radiation incident on the sample and focus radiation transmitted from the sample, is also disclosed.

Claims

1. A dual beam acousto-optic tunable spectrometer comprising;

a radiation source;

a birefringent acousto-optic tunable filter;

means for driving said acousto-optic tunable filter at a desired frequency such that radiation incident upon said filter is tuned to a first and second beam diverging from each other and the radiation outside the tuned bandwidth;

means for collecting said first tuned beam for use in analyzing a sample; and

means for collecting said second beam for use as a reference.

2. An acousto-optic tunable spectrometer comprising:

a radiation source;

means for collimating radiation from said radiation source;

an acousto-optic tunable filter;

means for driving said acousto-optic tunable filter at particular frequencies such that desired narrow bandwidths of radiation incident on said acousto-optic tunable filter will be tuned, said tuned bandwidth forming a first and second tuned beam which diverge from each other and the radiation outside said narrow bandwidth;

means for conveying said first tuned beam to a sample;

first detector means for detecting said first tuned beam after exposure to said sample;

second detector means for detecting said second tuned beam for use as a reference;

means for conveying said second tuned beam to said second detector;

analyzing means; and

means for inputing signals from said first and second detecting means to said analyzing means.

3. The spectrometer of claim 2, wherein said means for collimating radiation comprises a collimating lens.

4. The spectrometer of claim 3, wherein said tuned beams have an angle of diffraction upon exiting said acousto-optic tunable filter and said collimating lens has a field angle less than onehalf of said angle of diffraction.

5. The spectrometer of claim 3, further comprising condensing means between said radiation source and said collimating lens for collecting radiation from said radiation source.

6. The spectrometer of claim 5, wherein said condensing means comprises a pair of plano-convex lenses and a first aperture, said lenses focusing said radiation on said first aperture, said aperture defining the angular divergence of the radiation incident upon said collimating lens.

7. The spectrometer of claim 3, further comprising a first aperture between said source of radiation and said collimating lens for defining the angular divergence of the radiation incident upon said collimating lens.

8. The spectrometer of claim 6, further comprising a second aperture between said collimating lens and said acousto-optic tuned filter, said second aperture defining the size of the radiation beam incident upon the acousto-optic tunable filter.

9. The spectrometer of claim 8, wherein the size of the radiation beam incident upon the acousto-optic filter is slightly less than the size of the acousto-optic filter, such that the radiation beam incident upon the acousto-optic filter is not scattered prior to entering the filter.

10. The spectrometer of claim 3, further comprising a disc defining first and second tuned beam apertures, said first aperture for receiving said first tuned beam and said second aperture for receiving said second tuned beam, said disc further comprising a central region for absorbing said non-tuned radiation.

11. The spectrometer of claim 10, further comprising an achromatic lens system for collecting said radiation exiting said acousto-optic tunable crystal and focusing said first tuned beam on said first tuned beam aperture, focusing said second tuned beam on said second tuned beam aperture and focusing said nontuned beam on said central region of said disc.

12. The spectrometer of claim 11, wherein said achromatic lens system comprises an achromatic objective lens and an aplanatic meniscus lens.

13. The spectrometer of claim 10, wherein said means for conveying said first and second tuned beams comprises optical fibers, said spectrometer further comprising first and second condensing systems for collecting said first and second tuned beams received by said first and second tuned beam apertures, said first and second condensing systems focusing said first and second beams into said first and second optical fibers.

14. The spectrometer of claim 13, further comprising a cable for carrying said first and second optical fibers.

15. The spectrometer of claim 14, wherein said means for conveying said beam to said sample is an optical fiber.

16. The spectrometer of claim 3, further comprising a sample cell for holding said sample.

17. The spectrometer of claim 16, wherein said sample cell comprises a sample analysis area and a glass ball for collimating said first tuned beam on said sample analysis area.

18. The spectrometer of claim 17, wherein said sample cell comprises a glass ball for focusing radiation exposed to said sample on a collecting means.

19. The spectrometer of claim 18, wherein said collecting means is an optical fiber.

20. The spectrometer of claim 16, wherein said sample cell is remotely located from said system.

21. The spectrometer of claim 16, wherein said sample cell includes a leak detector.

22. The spectrometer of claim 16, wherein said sample cell includes a temperature sensor.

23. The spectrometer of claim 3, further comprising a sample cell for containing a sample to be tested, wherein said means for exposing said first tuned beam to a sample is a first optical fiber carrying said first tuned beam to said sample cell, said spectrometer further comprising a third optical fiber for conveying said first tuned beam from said sample cell to said first detector means.

24. The spectrometer of claim 23, wherein said first and second detector means comprise indium gallium arsenide or germanium.

25. The spectrometer of claim 24, wherein said first and second detectors further comprise silicon.

26. The spectrometer of claim 3, wherein said means for driving said acousto-optic tunable filter comprises a controller and transducer means in contact with said acousto-optic tunable filter, said transducer means controlled by said controller.

27. The spectrometer of claim 26, wherein said controller comprises a microprocessor for generating a code corresponding to a desired driving frequency of said acousto-optic tunable filter and a rf synthesizer for converting said code into a frequency for driving said transducer.

28. The spectrometer of claim 27, wherein said rf synthesizer comprises a low frequency synthesizer and a phase lock loop circuit for generating the frequency required to drive said transducer.

29. The spectrometer of claim 28, wherein said microprocessor accounts for deviations in the temperature of said acousto-optic tunable filter by generating a different code for driving said acousto-optic tunable filter at said desired frequency.

30. The spectrometer of claim 26, wherein said controller comprises a microprocessor.

31. The spectrometer of claim 30, wherein said microprocessor averages measurements to correct for acoustic resonances.

32. The spectrometer of claim 31, wherein said measurements are made in equal acoustic resonance wavelength increments above and below the desired frequency.

33. The spectrometer of claim 31, wherein said wavelength increment is one-quarter.

34. The spectrometer of claim 32, wherein one of said measurements is at the desired frequency and the other is onehalf acoustic resonance wavelength increment above the desired frequency.

35. The spectrometer of claim 27, wherein said microprocessor measures the signal at said detectors before generating a driving frequency, said measurements being used to correct subsequent sample and reference measurements.

36. An acousto-optic tunable spectrometer comprising;

a radiation source;

a collimating lens;

a first aperture between said radiation source and said collimating lens defining an angular divergence of radiation from said collimating lens;

a birefringent acousto-optic tunable filter for tuning a narrow bandwidth of incident radiation into a first and second tuned beam diverging from each other and the non-tuned radiation;

a microprocessor for determining a frequency for driving said acousto-optic tunable filter;

a second aperture between said acousto-optic tunable filter and said collimating lens, defining the boundary of the radiation incident on said acousto-optic tunable filter;

an achromatic lens system for focusing said first and second tuned beams onto a first and second aperture;

first and second optical fibers for collecting said tuned beams;

means for focusing said first and second beams from said first and second apertures into said first and second optical fibers;

a fluid sample cell including an analysis area bounding the sample to be analyzed, said first optical fiber attaching to said sample cell and providing said first tuned beam for analyzing said sample and means for collecting radiation transmitted and scattered by said sample and focusing said sample radiation on a third optical fiber;

a first detecting means for detecting said sample signal from said third optical fiber;

a second detecting means for detecting said second tuned beam from said second optical fiber;

means for conveying detected signals from said first and second detecting means to said microprocessor for analysis.

37. A method for the spectroscopic analysis of fluid samples comprising;

emitting infrared radiation;

collimating said radiation;

exposing said radiation to a birefringent acoustooptical tunable filter;

driving said acousto-optic tunable filter at a desired frequency to tune a specific narrow bandwidth of said radiation yielding a first and second diverging tuned beam;

isolating said first and second tuned beam from each other and the non-tuned radiation;

separately collecting raid first and second tuned beam;

applying said first tuned beam to a sample;

collecting the radiation transmitted and scattered by said sample;

detecting the collected radiation;

detecting the second tuned beam; and

determining the absorbance of the sample at the wavelength based on the value of the detected collected radiation and the value of the detected second tuned beam.