Digital gamma ray imaging device

• US 5,132,542 A
• Filed: 02/11/1991
• Issued: 07/21/1992
• Est. Priority Date: 02/11/1991
• Status: Expired due to Fees

• Current Assignee: The University of New Mexico
• Original Assignee: The University of New Mexico
• Inventors: Wolfe, David M., Bassalleck, Bernd, Hartshorne, Michael F., Mettler, Frederick A., Kelsey, Charles A.
• Primary Examiner(s): Hannaher, Constantine
• Assistant Examiner(s): Glick, Edward J.
• Application Number:
  US07/652,970
• Time in Patent Office: 526 Days
• Field of Search: 250/370.08, 250/370.09, 250/370.12, 250/370.13, 250/370.06, 250/363.03, 250/363.04, 250/363.05, 250/363.10
• US Class Current: 250/370.09
• CPC Class Codes: G01T 1/247 Detector read-out circuitry for processing gain or off-set correction H04N
• CPC Class Codes: G01T 1/2928 using solid state detectors

Abstract

The arrangement imaging a body through gamma radiation comprising the steps of detecting, within each fixed time period of a succession of fixed time periods at a plurality of locations impinged by the gamma radiation, electric charge levels corresponding to photoelectric events; counting within each fixed period only those charge levels at each location which are greater than a predetermined threshold level, and adding the counted charge levels for the succession of fixed time periods, whereby a distinct image of the body may be produced therefrom.

Claims

1. The method of providing selected image signals of a body through which gamma radiation from a source is passed, comprising the steps of:

a. detecting, within each fixed time period of a succession of fixed time periods at a plurality of locations impinged by the gamma radiation, electric charge levels corresponding to the energy level of the gamma radiation to be imaged, said electric charge levels thus being sufficient to cause a detectable response;

b. counting within each fixed time period from among the charge levels sufficient to cause a detectable response only those electric charge levels at each location which exceed a predetermined threshold level, said predetermined threshold level being approximately equal to the charge level of a photoelectric event which corresponds to an energy level at least higher than the energy level associated with Compton scattering, and

c. adding the counted electric charges for the succession of fixed time periods to provide selected signals representing an image of the body;

wherein uncounted charge levels and thus unwanted image signals are eliminated if they do not reach the threshold level within one of said fixed time periods.

2. The method of claim 1 wherein the source of gamma radiation is located within the body.

3. The method of claim 2 wherein the body is that of a human.

4. The method of claim 1 wherein the direction from which each location is impinged by the gamma radiation is essentially normal to the plane described by each location and the location immediately adjacent thereto.

5. The method of claim 1 wherein the locations are arranged in a multiplicity of rows and columns forming a two dimensional matrix.

6. Apparatus for providing selected image signals of a body through which gamma radiation from a source is passed, comprising:

a. means for detecting, within each fixed time period over a succession of fixed time periods at a plurality of locations impinged by gamma radiation, electric charge levels corresponding to the energy level of the gamma radiation to be imaged;

b. means for counting within each fixed time period from among the charge levels sufficient to cause a detectable response only those electric charge levels which exceed a predetermined threshold level, said predetermined threshold level being approximately equal to the charge level of a photoelectric even corresponding to an energy level at least higher than the energy level associated with Compton scattering, and

c. means for adding the counted charge levels for the succession of fixed time periods to provide selected signals representing an image of the body, whereby uncounted charge levels and thus unwanted image signals are eliminated if they do not reach the threshold level within one of said fixed time periods.

7. Apparatus as in claim 6 wherein said means for detecting comprises at each location a pixel of semiconductor material, said pixels being arranged in a multiplicity of rows and columns to form a two dimensional matrix.

8. Apparatus as in claim 7 wherein said means for detecting further comprises means for collimating the gamma radiation so that it impinges each pixel from a direction essentially normal to the plane described by the pixel and at least one immediately adjacent pixel in the matrix.

9. Apparatus as in claim 8 further comprising:

d. means for processing as signals the counted charge levels for the duration of the succession of fixed time periods to provide the basis for constructing an image of the body.

10. Apparatus as in claim 9 wherein the duration of the succession of fixed time periods is within the range of from approximately 10 seconds to approximately 10 minutes.

11. Apparatus as in claim 10 wherein the semiconductor material in each pixel has an atomic number exceeding 30.

12. Apparatus as in claim 8 wherein the semiconductor material in each pixel comprises a material selected from the group of materials including HgI₂, CdTe in passivated form, HgCdTe with implanted ions, GaAs, PbS, and pure Ge.