Frequency domain cross-correlation fluorometry with phase-locked loop frequency synthesizers

• US 4,840,485 A
• Filed: 07/27/1988
• Issued: 06/20/1989
• Est. Priority Date: 12/17/1986
• Status: Expired due to Term

• Current Assignee: ISS
• Original Assignee: ISS
• Inventors: Gratton, Enrico
• Primary Examiner(s): EVANS, FANNIE L
• Application Number:
  US07/225,595
• Time in Patent Office: 328 Days
• Field of Search: 356/317, 356/318, 356/417, 250/458.1, 250/459.1, 250/461.1, 250/461.2
• US Class Current: 356/317
• CPC Class Codes: G01N 21/6408 with measurement of decay time, time resolved fluorescence

Abstract

Frequency domain cross-correlation fluorometers may be improved over present designs by providing a coherent signal at one frequency to means for detecting luminescence from a sample, which is elicited by light modulated at another frequency, in which the two frequencies, obtained from a pair of phase-locked loop frequency synthesizers, are different from each other by at least 100 hertz, which is a significantly greater difference than used in corresponding prior art fluorometers. This permits the use of the phase-locked loop frequency synthesizers, rather than the currently used direct synthesis synthesizers, providing significant advantages.

Claims

1. Apparatus for cross-correlation frequency domain fluorometry, which comprises:

a source of electromagnetic radiation;

means for amplitude modulating the electromagnetic radiation at a first frequency;

means for directing the amplitude-modulated electromagnetic radiation at a sample;

means for detecting the luminescence of the sample;

means for providing a signal coherent with amplitude modulated signals produced by said amplitude modulating means, at a second frequency, to said detecting means;

means for modulating the gain of said detecting means by said signal;

said amplitude modulating means and means for providing a signal at a second frequency each comprising a separate phase-locked loop frequency synthesizer;

said second frequency being different from said first frequency by at least 100 hertz; and

means for deriving a resultant signal from said electromagnetic radiation and said detecting means at a frequency of the difference between said first and second frequencies, to detect phase shift and modulation changes of said luminescence from that of said electromagnetic radiation.

2. The apparatus of claim 1 in which the difference between said first and second frequencies is no less than 500 hertz.

3. The apparatus of claim 2 in which said first and second frequencies differ by 500 to 2000 hertz.

4. The apparatus of claim 1 in which said means for amplitude modulating the electromagnetic radiation at a first frequency includes Pockels cell means, driven by one of said phase-locked loop frequency synthesizers.

5. A method for frequency domain cross-correlation fluorometry, which comprises the steps of:

providing a source of electromagnetic radiation;

amplitude modulating the electromagnetic radiation at a first frequency with a Pockels cell driven by a phase-locked loop frequency synthesizer;

directing the amplitude-modulated electromagnetic radiation at a sample;

detecting with a detector the luminescence of the sample while modulating the gain of said detector with a signal at a second frequency to said detector;

with said signal at a second frequency being coherent with the modulation of said electromagnetic radiation and said second frequency being different from said first frequency by at least 100 hertz; and

deriving a resultant signal from said electromagnetic radiation and said detector at a frequency of the difference between said first and second frequencies, to detect phase shift and modulation of said luminescence from that of said electromagnetic radiation.

6. The method of claim 5 in which the difference between the first and second frequencies is no less than 500 hertz.

7. The method of claim 6 in which said first and second frequencies differ by 500 to 2000 hertz.

8. The method of claim 7 in which said electromagnetic radiation is modulated at said first frequency by Pockels cell means, driven by a phase-locked loop frequency synthesizer.

9. The method of claim 8 in which the gain of said detector is modulated at the second frequency by the signal from a phase-locked loop frequency synthesizer.