System and method for characterizing a sample by low-frequency spectra

• US 7,081,747 B2
• Filed: 08/20/2004
• Issued: 07/25/2006
• Est. Priority Date: 03/29/2002
• Status: Active Grant

• Current Assignee: Nativis, Inc.
• Original Assignee: Nativis, Inc.
• Inventors: Butters, John T., Butters, Lisa C., Butters, Bennett M.
• Primary Examiner(s): Patidar, Jay M.
• Application Number:
  US10/923,545
• Publication Number:
  US 20050030016A1
• Time in Patent Office: 704 Days
• Field of Search: 324247-249, 324/244, 324/228, 324/239, 600/409, 326/5, 505/162, 505845-846, 702 75- 77
• US Class Current: 324/248
• CPC Class Codes: G01N 37/005 Measurement methods not based on established scientific theories

Abstract

A method and apparatus for interrogating a sample that exhibits molecular rotation are disclosed. In practicing the method, the sample is placed in a container having both magnetic and electromagnetic shielding, and Gaussian noise is injected into the sample. An electromagnetic time-domain signal composed of sample source radiation superimposed on the injected Guassian noise is detected, and this signal is cross-correlated with a second time-domain signal produced by the same or similar sample, to produce a cross-correlated signal with frequency domain components. The latter is plotted in the frequency domain by a fast Fourier transform to produce a frequency domain spectrum in a frequency range within DC to 50 KHz. From this spectrum, one or more low-frequency signal components that are characteristic of the sample being interrogated are identified.

Claims

1. Apparatus for interrogating a sample that exhibits molecular rotation, comprising:

a container adapted for receiving the sample, the container having both magnetic and electromagnetic shielding;

a source of noise for injection into the sample, with the sample in the container;

a detector for detecting an electromagnetic time-domain signal composed of sample source radiation superimposed on the injected Gaussian noise;

a storage device for storing the time-domain signal and a second time-domain signal separately detected from the same or a similar sample; and

an electronic computer which is adapted to receive the stored signal from the storage device, and to process the signal by;

(i) cross correlating the time-domain signal detected with the second time-domain signal, to produce a frequency-domain spectrum in a frequency range within DC to 50 KHz, and

(ii) generating an output that includes information relating to spectral components in the spectrum that are characteristic of the sample.

2. The apparatus of claim 1, wherein the container is an attenuation tube having a sample-holding region, a magnetic shielding cage surrounding the region, and a Faraday cage contained within the magnetic shielding cage and also surrounding the region.

3. The apparatus of claim 1, wherein the sample container includes a temperature controller for maintaining the sample in the container at a selected temperature.

4. The apparatus of claim 1, wherein the source of noise includes a Gaussian noise generator and a Helmholz coil which is contained within the magnetic cage and the Faraday cage, and which receives a noise output signal from the noise generator.

5. The apparatus of claim 4, wherein the noise generator is designed to inject stationary white Gaussian noise into the sample, at an amplitude sufficient to produce non-stationary composite signal components.

6. The apparatus of claim 5, wherein the noise generator is designed to inject Gaussian noise into the sample at a frequency between DC and 2 KHz.

7. The apparatus of claim 1, wherein the detector is a first-derivative superconducting gradiometer which outputs a current signal, and a SQUID operatively connected to the gradiometer to convert the current signal to an amplified voltage signal.

8. The apparatus of claim 7, wherein the container is an attenuation tube having a sample-holding region, a magnetic shielding cage surrounding the region, and a Faraday cage contained within the magnetic shielding cage and also surrounding the region, the source of noise includes a Gaussian noise generator and a Helmholz coil which is contained within the magnetic cage and the Faraday cage, and which receives a noise output signal from the noise generator, and which further includes, for use in removing stationary noise components in the time-dependent signal, a signal inverter operatively connected to the noise source and to the SQUID, for receiving Gaussian noise from the noise source and outputting into the SQUID, Gaussian noise in inverted form with respect to the Gaussian noise injected into the sample.

9. The apparatus of claim 1, wherein the computer is operable to generate a frequency-domain spectrum in a range between DC to 6.5 Kz.

10. The apparatus of claim 9, wherein the computer is operable, to produce a frequency-domain signal in a range between 100 and 1,200 Hz.

11. The apparatus of claim 1, wherein the computer is operable, in generating an output, of identifying frequencies of low-frequency signal components in the spectrum whose cross-spectral correlations have a selected statistical measure above background spectral noise.

12. The apparatus of claim 11, for use in characterizing a known sample material in terms of its low-frequency signal components, wherein the computer is operable, in generating an output, of identifying material-specific low-frequency spectral components in the spectrum whose cross-spectral correlations have a selected statistical measure above background spectral noise.

13. The apparatus of claim 12, for use in identifying one or more components in a sample, wherein the computer is operable, in generating an output, to (a) identify frequencies of sample signal components (i) in a selected frequency range between DC and 50 KHz (ii) whose cross-spectral correlations have a selected statistical measure above background spectral noise, (b) compare such sample signal components with characteristic low-frequency signal components of known compounds suspected of being present in the sample, and (c) identify a compound as being present in the sample if its characteristic low-frequency signal frequencies correspond to those one or more of the sample-signal frequencies.

14. A method for interrogating a sample that exhibits molecular rotation, comprising:

placing the sample in a container having both magnetic and electromagnetic shielding;

injecting noise into the sample;

recording an electromagnetic time-domain signal composed of sample source radiation superimposed on the injected noise;

comparing the time-domain signal recorded with a second time domain signal separately recorded from the same or similar sample, to produce a frequency domain spectrum in a frequency range within DC to 50 Khz; and

identifying in the frequency-domain spectrum, one or more low-frequency signal components that are characteristic of the sample being interrogated.

15. The method of claim 14, wherein the injecting includes generating Gaussian noise from a noise generator and injecting the noise into the sample by means of a Helmholz coil which is located within the container.

16. The method of claim 15, wherein the injecting includes injecting stationary white Gaussian noise into the sample, at an amplitude sufficient to produce non-stationary composite signal components.

17. The method of claim 16, wherein the noise injected into the sample has a frequency between DC and 2 KHz.

18. The method of claim 14, wherein the detecting includes capturing the composite signal with a first-derivative superconducting gradiometer and converting the gradiometer signal to an amplified voltage signal by a SQUID.

20. The method of claim 14, which further includes transforming a cross-correlated frequency-domain spectrum to produce a frequency-domain spectral plot in a range between DC to 6.5 Kz.

21. The method of claim 20, which further includes transforming a cross-correlated frequency-domain spectrum to produce a frequency-domain spectral plot in a range between 100 and 1,200 Hz.

22. The method of claim 14, for use in characterizing a known sample material according to frequencies of its low-frequency signal components, which further includes identifying frequencies of sample-specific spectral components (i) in a selected frequency range between DC and 50 KHz (ii) whose cross-spectral correlations have a selected statistical measure above background spectral noise.

23. The method of claim 14, for use in identifying one or more components in a sample, which further includes (a) identifying the frequencies of sample spectral components (i) in a selected frequency range between DC and 50 KHz (ii) whose cross-spectral correlations have a selected statistical measure above background spectral noise, (b) comparing such sample spectral components with characteristic low-frequency spectral components of known compounds suspected of being present in the sample, and (c) identifying a compound as being present in the sample if one or more of its characteristic low-frequency spectral components correspond to one or more low-frequency spectral components of a known sample.

24. The method of claim 23, wherein the sample component is present in a liquid sample at a concentration between 1 part per million and 1 part per 10 billion.

25. The method of claim 24, wherein one or more of the low-frequency signal components of a compound exhibits a concentration-dependent frequency shift of less than 2 Hz, and the identifying includes approximating the concentration of a sample component by its frequency shift.

26. The method of claim 24, wherein one or more of the low-frequency signal components of a compound exhibits a concentration-dependent cross-spectral correlation, the identifying includes approximating the concentration of a sample component by its cross-spectral correlation.

19. The method of 18, wherein the container is an attenuation tube having a sample-holding region, a magnetic shielding cage surrounding the region, and a Faraday cage contained within the magnetic shielding cage and also surrounding the region, the noise is injected from a Gaussian noise generator and a Helmholz coil which is contained within the magnetic cage and the Faraday cage, and which receives a noise output signal from the noise generator, and which further includes, for use in removing stationary noise components in the time-dependent signal, a signal inverter operatively connected to the the noise source and to the SQUID, for receiving Gaussian noise from the noise source and outputting into the SQUID, Gaussian noise in inverted form with respect to the Gaussian noise injected into the sample.

27. A time-domain signal associated with a material of interest, produced by:

placing the sample of the material in a container having both magnetic and electromagnetic shielding,

injecting Gaussian noise into the sample; and

recording an electromagnetic time-domain signal composed of sample source radiation superimposed on the injected Gaussian noise, correlating the time-domain signal recorded with a second time domain signal separately recorded from the same or similar sample, to produce a correlated time-domain signal, and transforming the time-domain signal to a frequency domain spectrum in a frequency range within DC to 50 Khz, and identifying in the frequency-domain spectrum, one or more low-frequency signal components that are characteristic of the sample being interrogated.