Variable code gamma ray imaging system

• US 4,165,462 A
• Filed: 05/05/1977
• Issued: 08/21/1979
• Est. Priority Date: 05/05/1977
• Status: Expired due to Term

• Current Assignee: Albert Macovski, Dov Rosenfeld
• Original Assignee: Albert Macovski, Dov Rosenfeld
• Inventors: Macovski, Albert, Rosenfeld, Dov
• Primary Examiner(s): Smith, Alfred E.
• Assistant Examiner(s): Howell, Janice A.
• Application Number:
  US05/794,117
• Time in Patent Office: 838 Days
• Field of Search: 250/363 S, 250/369, 250/505, 250/514
• US Class Current: 250/363.04
• CPC Class Codes: G01T 1/295 using coded aperture devices, e.g. Fresnel zone plates handling of radiation of particles, e.g. using diaphragms, collimators, diffraction G21K1/00

Abstract

A gamma-ray source distribution in the body is imaged onto a detector using an array of apertures. The transmission of each aperture is modulated using a code such that the individual views of the source through each aperture can be decoded and separated. The codes are chosen to maximize the signal to noise ratio for each source distribution. These codes determine the photon collection efficiency of the aperture array. Planar arrays are used for volumetric reconstructions and circular arrays for cross-sectional reconstructions.

Claims

1. Apparatus for producing a three-dimensional tomographic image of a gamma-ray source comprising:

a detector array, producing an array of detector signals, for determining the position of each photon received from the source;

an aperture array positioned between the source and the detector array;

means for modulating the transmission of each of the apertures in the aperture array with an array of separable coding signals;

means for decoding the array of detector signals using an array of decoding signals which correspond to the separable coding signals to provide an array of projection signals representing the intensity of a projected image of the source through each aperture;

means for choosing the coding and decoding signals based on the intensity distribution of the source; and

means for utilizing the projection signals to produce a three-dimensional tomographic image of the source.

2. Apparatus as described in claim 1 wherein the means for choosing the coding and decoding signals is based on prior knowledge of the general size of the source distribution.

3. Apparatus as described in claim 1 wherein the means for choosing the coding and decoding signals is based on an initial analysis of the projection signals using initial coding and decoding signals.

4. Apparatus as described in claim 3 wherein the initial analysis of the projection signals provides a measure of the effective size of the source.

5. Apparatus as described in claim 4 wherein the measure of the effective size of the source includes calculating the ratio of the sum of the intensities of each element of the projected image to the maximum intensity of these elements.

6. Apparatus as described in claim 1 wherein the aperture array is a two-dimensional planar array and the detector array is a two-dimensional planar array parallel to the aperture array.

7. Apparatus as described in claim 1 wherein the aperture array is a circular ring and the detector array is a circular ring which is concentric with and has a larger diameter than that of the aperture array.

8. Apparatus as described in claim 7 wherein the means for modulating each of the apertures of the circular ring aperture array includes an additional circular ring concentric with and adjacent to the circular aperture array having coding apertures which define the coding signal and including means for rotating the additional circular ring.

9. Apparatus as described in claim 7 wherein the means for modulating each of the apertures of the circular ring aperture array includes a cylinder concentric with and adjacent to the circular aperture array having a plurality of rings of coding apertures with each ring defining a different coding signal and including means for rotating the cylinder to modulate the apertures and means for translating the cylinder axially to choose the desired coding signal based on the source distribution.

10. Apparatus as described in claim 7 including collimator plates between the source and the detector array to limit the photons reaching the detector to those representing a cross section of the source.

11. In a method for producing a three-dimensional tomographic image of a gamma-ray source the steps of:

imaging the source onto a detector array through an array of apertures to produce an array of detector signals;

modulating each of the apertures with an array of coding signals;

decoding the detector signals with an array of decoding signals corresponding to the coding signals to produce an array of projection signals representing the intensity of each element of a projected image of the source through each aperture;

selecting a set of coding and decoding signals based on the distribution of the source; and

reconstructing a three-dimensional tomographic view of the source using the projection signals.

12. The method of claim 11 wherein the step of selecting the coding and decoding signals is based on apriori knowledge of the general shape of the source.

13. The method of claim 11 wherein the step of selecting the coding and decoding signals is based on an initial analysis of the projection signals using initially chosen coding and decoding signals.

14. The method of claim 13 wherein the initial analysis of the projection signals provides an estimate of the size of the source.