Method of imaging a random medium

• US 5,137,355 A
• Filed: 06/08/1989
• Issued: 08/11/1992
• Est. Priority Date: 06/08/1988
• Status: Expired due to Term

• Current Assignee: The Research Foundation for The State University of New York (State University of New York)
• Original Assignee: The Research Foundation for The State University of New York (State University of New York)
• Inventors: Lubowsky, Jack, Aronson, Raphael, Barbour, Randall L.
• Primary Examiner(s): Rosenberger, Richard A.
• Application Number:
  US07/363,075
• Time in Patent Office: 1,160 Days
• Field of Search: 356/342, 356/237, 128/633, 128/664, 128/665, 250/358.1
• US Class Current: 356/342
• CPC Class Codes: G01N 2021/1782 In-depth resolution
• CPC Class Codes: G01N 2021/1793 Remote sensing
• CPC Class Codes: G01N 2021/4709 Backscatter
• CPC Class Codes: G01N 2021/4714 Continuous plural angles
• CPC Class Codes: G01N 21/4795 spatially resolved investigating of object in scattering medium in vivo A61B

Abstract

A non-invasive medical imaging technique capable of evaluating, in situ, the oxygenation state of body tissues (e.g., by measuring the spectral properties of heme proteins) is described. The technique is based on the measurement of scattered radiation in the near-infrared region (NIR), where significant penetration into body tissues occurs. The disclosed technique employs a multi-wavelength collimated source and a collimated receiver and performs a positional and angular scan of the scattered radiation for each position of the incident beam. The resultant data is evaluated by employing imaging schemes which give differential weights to the contribution of various volume elements (voxels) in the medium to the detector response. A three-dimensional spectroscopic image of the target medium is determined by considering the contribution of the various volume elements for each source-detector configuration and position of the incident beam at various frequencies. These measurements, in an imaging mode, yield vital physiological information while being, for example, a sensitive indicator of subtle physiological stress caused by disease or trauma.

Claims

1. A method for imaging a three-dimensional target object or other optical inhomogeneity in a turbid medium, comprising the steps of:

providing a substantially collimated beam of radiation and directing the beam onto a surface of a turbid medium containing a target object;

providing a substantially collimated receiver to receive scattered radiation;

performing positional scans comprising source-detector configurations having different source detector, separations and angles of the scattered radiation over the surface of the turbid medium at various separations and angles;

applying the data obtained from each positional scan to form a three-dimensional image of the target object by;

a. determining attenuation of emerging radiation from said target medium relative to a model medium;

b. determining a relative contribution of volume elements for each source-detector configuration;

c. superimposing the relative contribution of volume elements for all source-detector configurations;

d. obtaining a spectroscopic image;

e. displaying said spectroscopic image.

2. The method of claim 1, wherein said beam of radiation is near infrared radiation.

3. The method of claim 1, wherein said collimated receiver is a collimated receiver array.

4. The method of claim 3, wherein said receiver array includes collimated CCD detectors.

5. The method of claim 1, wherein said receiver is positioned for a reflectance measurement.

6. The method of claim 1, wherein said receiver is positioned for a transmission measurement.

7. The method of claim 1, wherein said positional scan includes having said collimated beam of radiation be laterally scanned.

8. The method of claim 1, wherein said positional scan includes a lateral translation of said collimated receiver.

9. The method of claim 1, wherein said positional scan includes an angular translation of said collimated receiver to provide differing angular information about the detector response.

10. The method of claim 1, wherein the data is applied to a data processing apparatus.

11. The method of claim 1, wherein said collimated receiver detects information regarding intensity of said scattered radiation.

12. The method of claim 1, wherein calculation of attenuation is performed by comparing measured values to expected values from a model medium calculated using Monte Carlo techniques.

13. The method of claim 12, wherein said weight function includes a calculation of a product of flux through a given voxel and an expected contribution of said voxel to a detector response.

14. The method of claim 1, wherein said attenuation step includes determining the ratio of actual data obtained from each positional scan to a calculated expected detection from said model medium.

15. The method of claim 1, wherein said determining relative contribution step includes multiplying said determined attenuation by a value of the weight function of each volume element for each source-detector configuaration under consideration.

16. The method of claim 1, wherein said superimposing step determines a three dimensional image of said target at a single frequency measurement.

17. The method of claim 1, wherein said model medium is simulated by assigning a weight to every point in the medium, wherein said weight is a product of the flux and expected contribution of a photon at a point to the detector response for a medium without an absorber.

18. The method of claim 1, wherein said imaging is used to evaluate, in situ, body tissue oxygenation state.

19. The method of claim 1, wherein said imaging is employed to measure spectroscopic properties of heme proteins, in situ.

20. The method of claim 1, wherein the substantially collimated beam of radiation is a multiple frequency beam.

21. The method of claim 20 wherein the multiple frequency beam is generated by C.W. or ultrafast pulse sources.

22. The method of claim 1, wherein steps a to c are repeated at various frequencies of radiation.

23. The method of claim 22, wherein the result of the superimposings at the various frequencies are superimposed.