Method and means for parallel frequency acquisition in frequency domain fluorometry

• US 5,257,202 A
• Filed: 11/27/1990
• Issued: 10/26/1993
• Est. Priority Date: 02/13/1989
• Status: Expired due to Term

• Current Assignee: Research Corporation Technologies
• Original Assignee: Research Corporation Technologies
• Inventors: Piston, David W., Feddersen, Brett A., Gratton, Enrico
• Primary Examiner(s): Cosimano, Edward R.
• Assistant Examiner(s): Ramirez, Ellis B.
• Application Number:
  US07/619,290
• Time in Patent Office: 1,064 Days
• Field of Search: 364/498, 364/553, 364/554, 364/728.03, 356/317, 356/318, 250/458.1
• US Class Current: 702/32
• CPC Class Codes: G01J 3/4406 Fluorescence spectrometry
• CPC Class Codes: G01N 21/6408 with measurement of decay time, time resolved fluorescence

Abstract

A digital frequency domain fluorometer utilizing a computer-controlled digital data acquisition system is use for the study of fluorescence and phosphorescence phenomena in the bio-chemical, biological and bio-physics arts. The computer is used for the direct collection of data, as well as for the filtering and calculation of the phase and modulation values of the sample under study. From these values, fluorescence lifetimes and anisotropy decay times can determined. The digital data acquisition system provides for the simultaneous collection and processing of several modulation frequencies. In addition, the digital frequency domain fluorometer can utilize an array detector for detecting the modulated light from the various samples under study. The use of the array detector provides a means for independently collecting data over a large number of pixels. This configuration allows for a time resolved image to be collected at once.

Claims

1. A digital frequency domain system for measuring the light emitted by a sample when excited by a light source having harmonic content, said system comprising:

(a) means for exciting said sample to emit a light signal, said means including a light source having a harmonic content and a predetermined fundamental frequency thereof;

(b) a first means for detecting the light emitted by the sample to generate a first electrical signal containing information representative of the response of said sample at said fundamental and harmonic frequencies;

(c) a second means for generating a second electrical signal representative of said fundamental frequency and a predetermined correlation frequency;

(d) cross-correlation means for mixing said first and second electrical signals to generate a third electrical signal having a response at the fundamental and harmonic frequencies imposed on said correlation frequency;

(e) means for digitizing said third electrical signal to obtain a plurality of data values for each period of the correlation frequency;

(f) a data processing means for simultaneously calculating from said plurality of data values the phase and modulation values of the response of the sample at the fundamental and a predetermined number of said harmonic frequencies.

2. A digital frequency domain system as claimed in claim 1 wherein the system further comprises a first digital filter means for removing any non-harmonic or non-synchronous frequencies from said plurality of data values.

3. A digital frequency domain system as claimed in claim 1 wherein the light signal emitted is fluorescence.

4. A digital frequency domain system as claimed in claim 1 wherein the light signal emitted is phosphorescence.

5. A digital frequency domain system as claimed in claim 2, 3 or 4 wherein the data processing means calculates a fast fourier transform on the plurality of data values.

6. A digital frequency domain system as claimed in claim 2, 3 or 4 wherein the cross-correlation means includes photomultiplier tube.

7. A digital frequency domain system as claimed in claim 2, 3 or 4 wherein said system further comprises means for polarizing said light source before said sample is excited.

8. A digital frequency domain system as claimed in claim 2, 3 or 4 wherein said light source is pulsed at a constant frequency.

9. A digital frequency domain system as claimed in claim 2, 3 or 4 wherein said system further includes a second light detecting means for generating a reference signal at said predetermined fundamental frequency.

10. A digital frequency domain fluorometer for measuring the fluorescent response of a sample when excited by a pulsed light source, said fluorometer comprising:

(a) means for exciting said sample to emit fluorescent light, said means including a pulsed light source of a predetermined fundamental frequency, said fundamental frequency intrinsically defining a plurality of harmonic frequencies;

(b) a first means for measuring the fluorescent light emitted by the sample to generate a first electrical signal containing phase and modulation information representative of the response of said sample at said fundamental and harmonic frequencies;

(c) a second means for generating a second electrical signal representative of said fundamental frequency and a predetermined correlation frequency;

(d) cross-correlation means for mixing said first and second electrical signals to generate a third electrical signal having the phase and modulation response at the fundamental and harmonic frequencies imposed on said correlation frequency;

(e) means for digitizing said third electrical signal to obtain a plurality of data values for each period of the correlation frequency;

(f) a first filter means for removing any non-harmonic or non-synchrous frequencies from said plurality of data values;

(g) a data processing means for calculating a fast fourier transform on said plurality of data and modulation values to obtain the phase values of the response of the sample at the fundamental and a predetermined number of said harmonic frequencies;

11. A digital frequency domain fluorometer as claimed in claim 10 which further comprises means for polarizing said pulsed light source before said sample is excited.

12. A digital frequency domain fluorometer as claimed in claim 10 which further comprises means for generating a reference beam of pulsed light at said predetermined fundamental frequency, and means for generating a fourth electrical signal in response to said reference beam.

13. A digital frequency domain fluorometer as claimed in claim 12 wherein said cross-correlation means mixes said second and fourth electrical signals to generate a fifth electrical reference signal at the correlation frequency.

14. A digital frequency domain fluorometer as claimed in claim 13 wherein said means for digitizing also digitizes said fifth electrical reference signal for use by said data processing means in calculating said fast fourier transforms.

15. A digital frequency domain fluorometer as claimed in claim 10 wherein said cross-correlation means is a photomultiplier tube.

16. A digital frequency domain fluorometer as claimed in claim 11, which further comprises means for polarizing said emitted light at two orthogonal angles.

17. A digital frequency domain fluorometer as claimed in claim 16 wherein said data processing means computes the anisotropic decay from the phase and modulation values obtained from said orthogonal polarizations.

18. A digital frequency domain fluorometer as claimed in claim 10 wherein said system further comprises means for varying the wave length of the emitted light.

19. A digital frequency domain fluorometer as claimed in claim 10 wherein said pulsed light source has a wave length in the UV range.

20. A method of measuring the response of a sample having a harmonic content when excited by a light source, said method comprising:

(a) exciting said sample to emit a light signal with a light source at a predetermined fundamental frequency, said light source having a harmonic content;

(b) detecting the light emitted by the sample to generate a first electrical signal containing information representative of the response of said sample at said fundamental and harmonic frequencies;

(c) generating a second electrical signal representative of said fundamental frequency and a predetermined correlation frequency;

(d) mixing said first and second electrical signals to generate a third electrical signal having a response at the fundamental and harmonic frequencies imposed on said correlation frequency;

(e) digitizing said third electrical signal to obtain a plurality of data values for each period of the correlation frequency;

(f) simultaneously calculating from said plurality of data values, the phase and modulation values of the response of the sample at the fundamental and a predetermined number of said harmonic frequencies.

21. A method of measuring the response of a sample as claimed in claim 20, wherein the method further includes the step of removing any non-harmonic or non-synchronous frequencies from said plurality of data values, prior to the calculation of the fast fourier transform.

22. A method of measuring the response of a sample as claimed in claim 20, wherein the light signal emitted by the sample is fluorescence.

23. A method of measuring the response of a sample as claimed in claim 20, wherein the light signal emitted by the sample is phosphorescence.

24. A method of measuring the response of a sample as claimed in claim 20 or 21 or 22 which further includes the step of polarizing the light source prior to the excitation of the sample.

25. A method of measuring the response of a sample as claimed in claim 24 which further includes the step of polarizing the emitted light at an orthogonal angle to said first polarization.

26. A method of measuring the response of a sample as claimed in claim 20 or 21 or 22 wherein the method includes the step of pulsing the light source at a constant frequency.

27. A method of measuring the response of a sample as claimed in claim 20 or 21 or 22 wherein the method further includes the steps of:

(a) generating a reference beam from said light source;

(b) mixing a fourth electrical signal generated by said reference beam with said second electrical signal to create a reference signal at the correlation frequency, and;

(c) digitizing the reference signal to obtain a plurality of reference data values to be used in calculating the phase values of the response of the sample.

28. A method of measuring the response of a sample as claimed in claim 20 or 21 or 22 wherein said excitation step is conducted with a light source having a UV wave length.

29. A method of measuring the response of a sample as claimed in claim 20 or 21 or 22 wherein said detecting step and said mixing step are conducted simultaneously with a photomultiplier tube.

30. A digital frequency domain fluorometer for measuring the response of a sample when excited by a light source, said fluorometer comprising:

(a) first means for exciting said sample to emit a light signal, said means including a light source having a harmonic content and a predetermined fundamental frequency, said light signal containing phase and modulation information representative of the response of the sample at said fundamental and harmonic frequencies;

(b) second means for generating a second signal representative of said fundamental frequency and a predetermined correlation frequency;

(c) third means for mixing said light signal and said second signal to generate a third signal representative of the phase and modulation information imposed on the correlation frequency;

(d) fourth means for converting third signal to an electrical signal and digitizing said electrical signal to obtain a plurality of data values for each period of the correlation frequency;

(e) a data processing means for simultaneously calculating from said plurality of data values phase and modulation values of the response of the sample at the fundamental and a predetermined number of said harmonic frequencies.

31. A digital frequency domain fluorometer as claimed in claim 30 wherein said third means includes an image intensifier which is gated by said second signal.

32. A digital frequency domain fluorometer as claimed in claim 31 wherein said fourth means is an array detector.

33. A digital frequency domain fluorometer as claimed in claim 30 or 31 or 32 wherein the light signal is a fluorescence signal.

34. A digital frequency domain fluorometer as claimed in claim 30 or 31 or 32 wherein the light signal is a phosphorescence signal.

35. A digital frequency domain fluorometer as claimed in claim 30 wherein said device further includes a digital averaging filter.

36. A digital frequency domain fluorometer as claimed in claim 30 or 31 or 32 or 35 wherein said data processing means calculates a fast fourier transform on the plurality of data values.

37. A digital frequency domain fluorometer as claimed in claim 36 wherein the fluorometer further includes means for polarizing the light source before the sample is excited.

38. A digital frequency domain fluorometer as claimed in claim 30 or 31 or 32 wherein the light source is pulsed at a constant frequency.

39. A digital frequency domain fluorometer as claimed in claim 30 or 31 or 32 wherein the light source is modulated at said predetermined fundamental frequency.

40. An improved array detector for detecting the emissions of an excited sample, said array detector

(a) means for exciting a sample said means exciting said sample at a predetermined frequency f₁ ;

(b) an array detector for receiving and recording the level of emissions received from sample;

(c) an image intensifier positioned between said sample and said detector;

(d) means for selectively biasing said image intensifier to effectively gate the emissions received by said detector at a frequency of f₁ and f_c ;

(e) means for reading the recorded levels of emissions at the array detector at a frequency greater than f_c

41. A system for measuring the light emitted by a sample when excited by a light source, said system having an array detector for detecting the modulated light emissions of an excited sample, said array detector comprising:

(a) a semiconductor array, for receiving and recording the level of modulated light emissions received from said sample;

(b) an image intensifier positioned between the sample and said semiconductor array, said image intensifier modulating the gain of the modulated light emissions received from said sample and translating said emissions from a first frequency range to a second frequency range;

(c) means for selectively biasing said image intensifier to effectively pass to said array detector emissions having frequencies of f₁ and f_c ; and

(d) means for reading at a frequency than f_c, the recorded levels of modulated light emissions of said array detector.

42. The array detector as claimed in claim 41 further comprising means for coupling said semiconductor array with said image intensifier, said array detector translates said modulated light emissions into electrical signals while maintaining a spatial geometry equivalent to said modulated light emissions.

43. The array detector as claimed in claim 42 wherein said spatial geometry is maintained on a pixel by pixel geometry in an X-Y plane thus allowing the emissions from said sample to be studied at discrete X-Y locations.

44. The array detector as claimed in claim 43 wherein said coupling means comprises an optical fiber coupler.

45. The array detector as claimed in claim 44 wherein said semiconductor array is a charged-coupled device.

46. The array detector as claimed in claim 44 wherein said semiconductor array is a diode array.

47. The array detector as claimed in claim 41 wherein said image intensifier translates the modulated light emission received from said sample from said first frequency range to said second frequency range by modulating the gain of said emissions utilizing a radio frequency modulating signal.

48. The array detector as claimed in claim 47 wherein said first frequency range is the mega hertz frequency range and said second frequency range is the hertz frequency range.

49. The array detector as claimed in claim 48 wherein said modulation is a heterodyning technique for the frequency translation of said modulating light emissions received from said sample to a frequency range for display and recording by said array detector.

50. The array detector as claimed in claim 49 wherein said means for selectively biasing said image intensifier is a circuit for adjusting the modulation gain of said image intensifier.

51. A system for measuring the light emitted by a sample when excited by a light source, said system having an array detector for detecting the modulated light emissions of an excited sample, said array detector comprising:

(a) a semiconductor array for receiving and recording the level of modulated light emissions received from said sample;

(b) an image intensifier positioned between said sample and said semiconductor array, said image intensifier modulating the gain of the modulated light emissions from a first frequency range to a second frequency range;

(c) means for selectively biasing said image intensifier to effectively pass to said array detector emissions having frequencies of f₁ and f_c ;

(d) a modulator means for further modulating said modulated light emissions from said sample at said frequency f_c ; and

(e) means for reading at a frequency other than f_c, the recorded levels of modulated light emissions of said array detector.

52. The array detector as claimed in claim 51 further comprising means for coupling said semiconductor array with said image intensifier, said array detector translates said modulated light emissions into electrical signals while maintaining a spatial geometry equivalent to said modulated light emissions.

53. The array detector as claimed in claim 52 wherein said spatial geometry is maintained on a pixel by pixel geometry in an X-Y plane thus allowing the emissions from said sample to be studied at discrete X-Y locations.

54. The array detector as claimed in claim 51 wherein said image intensifier translates the modulated light emission received from said sample from said first frequency range to said second frequency range by modulating the gain of said emissions utilizing a radio frequency modulating signal.

55. The array detector as claimed in claim 54 wherein said first frequency range is the mega hertz frequency range and said second frequency range is the hertz frequency range.

56. The array detector as claimed in claim 55 wherein said modulation is a heterodyning technique for the frequency translation of said modulating light emissions received from said sample to a frequency range for display and recording by said array detector.

57. The array detector as claimed in claim 56 wherein said heterodyning technique utilizes a unique gating technique which cross-correlates a high frequency source at f₁ with said image intensifier at a frequency of f₁ +f_c to optically cross-correlate the fluorescence emission response phase and modulation information onto f_c, resulting in a heterodyned signal.

58. The array detector as claimed in claim 57 wherein said modulator means is a mechanical chopper phase locked with the modulation frequency of said intensifier, a modulated output from said mechanical chopper is mixed with said heterodyned signal resulting in a DC signal.

59. The array detector as claimed in claim 58 wherein said semiconductor array detects said DC signal to record one point of a low frequency sine wave from which phase and demodulation of the emitted signal is derived.

60. The array detector as claimed in claim 58 wherein said mechanical chopper is phase shifted a predetermined number of times in order to collect a series of points of said low frequency sine wave from which phase and demodulation of the emitted signal can be derived.

61. The array detector as claimed in claim 51 wherein said means for selectively biasing said image intensifier is a circuit for adjusting the modulation gain of said image intensifier.

62. An array detector for detecting the modulated light emissions of an excited sample, said array detector comprising:

(a) a semiconductor array for receiving and recording the level of modulated light emission received from said sample;

(b) an image intensifier positioned between said sample and said semiconductor array, said image intensifier modulating the gain of the modulated light emissions from a first frequency range to a second frequency range;

(c) means for selectively biasing said image intensifier to effectively pass to said array detector emissions having frequencies of f₁ and f_c ;

(d) a modulator means for further modulating said modulated light emissions from said sample at said frequency f_c ; and

(e) means for reading at a frequency other than f_c, the recorded levels of modulated light emissions of said array detector.

63. The array detector as claimed in claim 62 further comprising means for coupling said semiconductor array with said image intensifier, said array detector translates said modulated light emissions into electrical signals while maintaining a spatial geometry equivalent to said modulated light emissions, said spatial geometry is maintained on a pixel by pixel geometry in an X-Y plane thus allowing the emissions from said sample to be studied at discrete X-Y locations.

64. The array detector as claimed in claim 63 wherein said image intensifier translates the modulated light emission received from said sample from the mega hertz frequency range to the hertz frequency range by modulating the gain of said emissions utilizing a radio frequency modulating signal, said modulation is a heterodyning technique for the frequency translation of said modulating light emissions received from said sample to a frequency range for display and recording by said array detector, said heterodyning technique utilizes a unique gating technique which cross correlates a high frequency source at f₁ +f_c to phase and modulation information onto f_c, resulting in an heterodyned signal.

65. The array detector as claimed in claim 64 wherein said modulator means is a mechanical chopper phase locked with the modulation frequency of said intensifier, a modulated output from said mechanical chopper is mixed with said heterodyned signal resulting in a DC signal, said semiconductor array detects said DC signal to record one point of a low frequency sine wave from which phase and demodulation of the emitted signal is derived, said mechanical chopper is phase shifted a predetermined number of times in order to collect a series of points of said low frequency sine wave from which phase and demodulation of the emitted signal can be derived.