Interferometric apparatus and method for detection and characterization of particles using light scattered therefrom

• US 4,764,013 A
• Filed: 03/23/1987
• Issued: 08/16/1988
• Est. Priority Date: 03/23/1987
• Status: Expired due to Fees

• Current Assignee: The United States of America As Represented By The Secretary of Agriculture
• Original Assignee: United States Department of Energy (Government of the United States of America)
• Inventors: Johnston, Roger G.
• Primary Examiner(s): Willis, Davis L.
• Assistant Examiner(s): Koren, Matthew W.
• Application Number:
  US07/028,987
• Time in Patent Office: 512 Days
• Field of Search: 356/336, 356/338, 356/340, 356/364, 356/368, 356/349, 250/225
• US Class Current: 356/484
• CPC Class Codes: G01J 2009/0207 Double frequency, e.g. Zeeman
• CPC Class Codes: G01J 9/04 by beating two waves of a same source but of different frequency and measuring the phase shift of the lower frequency obtained
• CPC Class Codes: G01N 15/0205 by optical means
• CPC Class Codes: G01N 15/0211 Investigating a scatter or diffraction pattern
• CPC Class Codes: G01N 15/14 Optical investigation techniques, e.g. flow cytometry
• CPC Class Codes: G01N 2021/4792 Polarisation of scatter light
• CPC Class Codes: G01N 21/21 Polarisation-affecting properties G01N21/19 takes precedence

Abstract

Interferometric apparatus and method for detection and characterization of particles using light scattered therefrom. Differential phase measurements on scattered light from particles are possible using the two-frequency Zeeman effect laser which emits two frequencies of radiation 250 kHz apart. Excellent discrimination and reproducibility for various pure pollen and bacterial samples in suspension have been observed with a single polarization element. Additionally, a 250 kHz beat frequency was recorded from an individual particle traversing the focused output from the laser in a flow cytometer.

Claims

1. Apparatus for the indentification and characterization of particles in a sample by observing light scattered therefrom, comprising in combination:

means for producing a first radiation having a first wavelength and a first polarization;

means for producing a second radiation substantially collinear with said first radiation and having a second wavelength and a second polarization substantially orthogonal to said first polarization;

containment means containing said sample, for allowing said first and second radiations to scatter from collisions with said particles in said sample;

polarization means receiving scattered first and second radiations for resolving said scattered first and second radiations, said polarization means having an axis of transmission along which resolved scattered first and second radiations pass;

photodetector means receiving and detecting said resolved scattered first and second radiations for outputting a beat frequency resulting from interaction between said resolved scattered first and second radiations, said beat frequency having a relative phase and amplitude; and

measurement means receiving said beat frequency for measuring and outputting said relative phase of said beat frequency, for use in identifying and characterizing said particles.

2. The apparatus as described in claim 1, further comprising measurement means for measuring and outputting said amplitude of said beat frequency, for use in identifying and characterizing said particles.

3. The apparatus as described in claim 2, further comprising means for moving a combination of said polarization means and said photodetector means about said containment means to measure and output said relative phase and said amplitude of said beat frequency as functions of scattering angle.

4. The apparatus as described in claim 1, further comprising means located intermediate said containment means and said photodetector means for defining the volume of said scattered first and second radiations.

5. The apparatus as described in claim 1, wherein said first polarization and said second polarization comprise linear polarizations.

6. The apparatus as descried in claim 5, wherein the angle of said axis of transmission of said polarization means with respect to the axis of said first polarization is selected from the group comprising 0°

, 45°

, and 90°

.

7. The apparatus as described in claim 1, wherein said means for producing a first radiation and said means for producing a second radiation comprise laser means.

8. The apparatus as described in claim 7, wherein said first and second radiations have a difference frequency of not more than 100 MHz.

9. The apparatus as described in claim 8, wherein said difference frequency is stable to at least 0.1 parts per million.

10. The apparatus as described in claim 7, wherein said laser means comprises a two-frequency Zeeman effect laser.

11. The apparatus as described in claim 1, wherein said first polarization and said second polarization comprise circular polarizations.

12. The apparatus as described in claim 11, wherein said polarization means includes a circular polarizer.

13. A method for identifying and characterizing particles in a sample by observing light scattered therefrom, which comprises the steps of:

producing a first radiation having a first wavelength and a first polarization;

producing a second radiation substantially collinear with said first radiation and having a second wavelength and a second polarization substantially orthogonal to said first polarization;

scattering said first and second radiations by irradiating said sample with said first and second radiations;

receiving and resolving scattered first and second radiations along an axis of transmission having a predetermined polarization angle, and outputting resolved scattered first and second radiations;

detecting said resolved scattered first and second radiations, said detection producing a beat frequency, having a relative phase and amplitude, from the interaction of said resolved scattered first radiation with said resolved scattered second radiation, and outputting said beat frequency;

measuring said relative phase of said beat frequency; and

outputting said relative phase for use in identifying and characterizing said particles.

14. The method as described in claim 13, further comprising the steps of measuring and outputting said amplitude of said beat frequency.

15. The method as described in claim 14, further comprising the steps of measuring said relative phase and said amplitude of said beat frequency at a plurality of scattering angles, and outputting said relative phase and said amplitude of said beat frequency as functions of said plurality of scattering angles.

16. The method as described in claim 13, further comprising the step of defining the volume of said scattering first and second radiations after the step of scattering said first and second radiations, and again after the step of outputting resolved scattered first and second radiations.

17. The method as described in claim 13, wherein said first and second radiations comprise laser radiations.

18. The method as described in claim 17, wherein the difference frequency between said first wavelength and said second wavelength is not more than 100 MHz.

19. The method as described in claim 18, wherein said difference frequency is stable to at least 0.1 parts per million.

20. The method as described in claim 17, wherein said laser radiations comprise two-frequency Zeeman effect laser radiations.

21. The method as described in claim 13, wherein said first polarization and said second polarization comprise linear polarizations.

22. The method as described in claim 21, wherein said predetermined polarization angle with respect to the axis of said first polarization is from the group comprising 0°

, 45°

, and 90°

.

23. The method as described in claim 13, wherein said first polarization and said second polarization comprise circular polarizations;

24. The method as described in claim 23, wherein said step of receiving and resolving said scattered first and second radiations includes resolving said scattered first and second radiation into circularly polarized scattered first and second radiations.

29. The apparatus as described in claim 24, wherein said first and second radiations have a difference frequency of no more than 100 MHz.

30. The apparatus as described in claim 29, wherein said difference frequency is stable to at least 0.1 parts per million.

25. Apparatus for the indentification and characterization of individual particles in a flow by observing light scattered therefrom, comprising in combination;

means for producing a first radiation having a first wavelength and a first polarization;

means for producing a second radiation substantially collinear with said first radiation and having a second wavelength and a second polarization substantially orthogonal to said first polarization;

containment means controlling the flow of said individual particles for allowing said first and second wavelengths to scatter from collisions with said individual particles;

polarization means receiving scattered first and second radiations for resolving said scattered first and second radiations, said polarization means having an axis of transmission along which resolved scattered first and second radiations pass;

photodetector means receiving and detecting said resolved scattered first and second radiations for outputting the beat frequency resulting from the interaction between said resolved scattered first and second radiations, said beat frequency having a relative phase and amplitude; and

measurement means receiving said beat frequency for measuring and outputting said relative phase as a function of time for use in identifying and characterizing said individual particles.

26. The apparatus as described in claim 25, further comprising means for measuring and outputting said amplitude of said beat frequency as a function of time for use in identifying and characterizing said individual particles.

27. The apparatus as described in claim 26, further comprising means for measuring and outputting said relative phase and said amplitude of said beat frequency as functions of time at a plurality of scattering angles.

28. The apparatus as described in claim 25, wherein said means for producing said first and second radiations comprise laser means.

31. The apparatus as described in claim 28, wherein said laser means comprises a two-frequency Zeeman effect laser.

32. The apparatus as described in claim 25, wherein said first polarization and said second polarization comprise linear polarizations.

33. The apparatus as described in claim 32, wherein the angle of said axis of transmission of said polarization means with respect to the axis of said first polarization is selected from the group comprising 0°

, 45°

, and 90°

.

34. The apparatus as described in claim 25, wherein said first polarization and said second polarization comprise circular polarizations.

35. The apparatus as described in claim 34, wherein said polarization means comprises a circular polarizer.

36. The apparatus as described in claim 25, further comprising focusing means for reducing the diameter of said first and second radiations prior to collision with said individual particles.

37. The apparatus as described in claim 25, further comprising light gathering means intermediate of said containment means and said polarization means for maximizing collection of said scattered first and second radiations.

38. The apparatus as described in claim 25, further comprising slit means intermediate of said containment means and said polarization means, for improving spatial resolution of said scattered first and second radiations.

39. A method for identifying and characterizing individual particles in a flow by observing light scattered therefrom, comprising the steps of:

producing a first radiation having a first wavelength and a first polarization;

producing a second radiation substantially collinear with said first radiation and having a second wavelength and a second polarization substantially orthogonal to said first polarization;

scattering said first and second radiations by irradiating said particles in a flow with said first and second radiations;

receiving and resolving scattered first and second radiations along an axis of transmission having a predetermined polarization angle, and outputting resolved scattered first and second radiatons;

detecting said resolved scattered first and second radiations, said detection producing a beat frequency, having a relative phase and amplitude, from the interaction of said resolved scattered first radiation with said resolved scattered second radiation, and outputting said beat frequency;

measuring said relative phase of said beat frequency as function of time; and

outputting said relative phase of said beating frequency as a function of time for use in identifying and characterizing said individual particles.

40. The method as described in claim 39, further comprising the steps of measuring and outputting said amplitude of said beat frequency as a function of time for use in identifying and characterizing said individual particles.

41. The method as described in claim 40, further comprising the step of measuring said relative phase and said amplitude as functions of time at a plurality of scattering angles, and outputting said relative phase and said amplitude as functions of time and of said scattering angles.

42. The method as described in claim 39, wherein said first polarization and said second polarization comprise linear polarizations.

43. The method as described in claim 42, wherein said predetermined polarization angle with respect to the axis of said first polarization is chosen from the group comprising 0°

, 45°

, and 90°

.

44. The method as described in claim 39, wherein said first and second radiations comprise laser radiations.

45. The method as described in claim 44, wherein the difference frequency between said first wavelength and said second wavelength is not more than 100 MHz.

46. The method as described in claim 45, wherein said difference frequency is stable to at least 0.1 parts per million.

47. The method as described in claim 44, wherein said laser radiations comprise two-frequency Zeeman effect laser radiations.

48. The method as described in claim 39, wherein said first polarization and said second polarization comprise circular polarizations.

49. The method as described in claim 48, wherein said step of receiving and resolving said scattered first and second radiations further comprises resolving said scattered first and second radiations into circularly polarized scattered first and second radiations.

50. The method as described in claim 39, further comprising the step of reducing the beam diameter of said first and second radiations before being scattered by said particles in a flow.

51. The method as described in claim 39, further comprising the step of optically collecting said scattered first and second radiations before said step of receiving and resolving said scattered first and second radiations.