Multimedia detectors for medical imaging

• US 6,207,958 B1
• Filed: 08/10/1998
• Issued: 03/27/2001
• Est. Priority Date: 02/12/1996
• Status: Expired due to Fees

• Current Assignee: University of Akron
• Original Assignee: University of Akron
• Inventors: Giakos, George C.
• Primary Examiner(s): Ham, Seungsook
• Assistant Examiner(s): HANIG, RICHARD E
• Application Number:
  US09/117,925
• Time in Patent Office: 960 Days
• Field of Search: 250/385.1, 250/394, 250/374, 250/370.01, 250/375, 250/372.R
• US Class Current: 250/385.1
• CPC Class Codes: G01T 1/185 with ionisation chamber arrangements
• CPC Class Codes: G01T 1/2935 using ionisation detectors
• CPC Class Codes: H01J 47/02 Ionisation chambers

Abstract

The application of gas-detection principles on both dual-energy detection, such as for chest radiography and mammorgraphy, and quantitative autoradiography enhances dramatically the image quality of the digital dual-energy detector with great implications in general-purpose digital radiography, computer assisted tomography (CT), microtomography and x-ray microscopy, and offers notable advantages over film autoradiography with a higher sensitivity, much lower exposure times, as well as imaging access at the cellular level. A gas microstrip detector receives incident radiation through a subject to generate an image. The detector includes a substrate having on a first surface a plurality of alternating anodes and cathodes, a detector cathode spaced apart from and opposing the substrate, and a zone for dispensing a gaseous medium between the substrate and the detector cathode and for receiving incident radiation imparted through the subject.

Claims

1. A gas microstrip detector which receives incident radiation through a subject to generate an image, comprising:

a substrate having a first surface;

a plurality of alternating anodes and cathodes disposed on said first surface;

a plurality of electrodes disposed on an opposite surface of said substrate and oriented substantially perpendicularly with respect to said plurality of alternating anodes and cathodes, said plurality of electrodes separated into a front zone and a back zone;

a detector cathode spaced apart from and facing said first surface; and

a zone for disposing a gaseous medium between said substrate and the detector cathode and for receiving incident radiation imparted through the subject, wherein said front zone generates a first image signal and said back zone generates a second image signal for comparison to said first image signal.

2. The detector of claim 1, wherein the gaseous medium is selected from the group consisting of argon, xenon, krypton, and mixtures thereof, and at least one of argon, xenon, krypton and their mixtures in combination with at least one of a polar and a quenching compounds.

3. The detector of claim 2 wherein the gaseous medium is maintained at a predetermined pressure in a direct ionization mode to provide a high quantum efficiency and a reduced electron range.

4. The detector of claim 1, wherein the incident radiation is imparted from a scanning beam geometry.

5. The detector of claim 1, further comprising an imaging system for receiving and processing said first and second image signals.

6. The detector of claim 1, wherein said plurality of alternating anodes and cathodes are photolithographically disposed on the substrate.

7. The detector of claim 6, wherein said substrate is at least partially insulated and wherein a Kumakhov lens or a plurality of capillary optics is coupled with said substrate to provide an enhanced image.

8. The detector of claim 6 further comprising a neutral zone between said front and back zones, the neutral zone facilitating a distinction between the first and second image signals.

9. The detector of claim 6 further comprising:

a pre-filter for producing a bimodal x-ray spectrum that is passed through the subject; and

a detector housing which carries a window through which the bimodal x-ray spectrum is passed, wherein the substrate is received within the detector housing.

10. The detecotr of claim 1, wherein the detector cathode is disposed between a radioactive plate source and the substrate to provide means for quantitative autoradiography.

11. The detector of claim 10, wherein said radioactive plate source emits a predetermined level of radiation to ionize said gas detection medium.

12. The detector of claim 1 further comprising:

a photo-tube for receiving the substrate and filled with the gaseous medium to implement positron emission tomography, gamma camera, computer tomography or single photon emission tomography.

13. The detector of claim 12 further comprising:

a primary detection region and a transfer gap within the photo-tube; and

a readout circuit coupled to the phototube to generate an image.

14. The detector of claim 13 further comprising:

a radiation source adjacent said photo-tube for generating radiation and providing a start pulse to said readout circuit;

a crystal for absorbing radiation from said radiation source and generating scintillation light for ionizing the gaseous medium which generates a plurality of photoelectrons in an adjacent conversion zones;

a preamplification grid adjacent said conversion zone to multiply said plurality of electrons;

a mesh between said preamplification grid and said substrate to register a coincidence event and generate a stop plus received by said readout circuit wherein said detector generates a position reading and said readout circuit, determines a difference between said start and stop pulses for association with said position reading.

15. The detector according to claim 1 further comprising

a semiconductor substrate disposed between the substrate and a plate wherein a voltage is applied between the plate and said plurality of electrodes, and wherein said gas medium is encapsulated at a predetermined pressure.

16. The detector according to claim 15 wherein electrons are produced by direct x-ray ionization of the semiconductor substrate and are drifted toward the first plurality of anode strips to generate the image and wherein the incident radiation is imparted from a scanning beam geometry.

17. The detector according to claim 1 further comprising

a photosensitive coating disposed over the substrate wherein said substrate is coupled to means for generating light that is exposed to the incident radiation, and wherein said gas medium is encapsulated at a predetermined pressure.

18. The detector according to claim 17 wherein said means for generating light is a scintillation crystal carried by a window of a detector housing.

19. The detector according to claim 1 further comprising

a detector housing providing a window which receives one of a scintillator crystal and a fiber optic plate, said housing also receiving said substrate;

and

a photosensitive coating disposed on a surface of one of said scintillator crystal and said fiber optic plate.

20. The detector according to claim 17 wherein said means for generating light is a plurality of scintillating fibers coupled to the photosensitive coating and carried in a detector housing.

21. A method for obtaining an image of a subject exposed to incident radiation comprising the steps of:

exposing a detector to incident radiation projected through a sample,

wherein the detector comprises a gas microstrip detector, including

a substrate having on a first surface a plurality of alternating anodes and cathodes,

a detector cathode spaced apart from and opposing the substrate first surface,

a plurality of electrodes disposed on an opposite surface of said substrate and oriented substantially perpendicularly with respect to said plurality of alternating anodes and cathodes, said plurality of electrodes separated into a front zone and a back zone, and

a zone for disposing a gaseous medium between the substrate and the detector cathode and for receiving incident radiation from the sample, wherein the incident radiation produces photons by ionization of the gaseous medium;

absorbing the photons in said detector, by applying an electric field between the detector cathode and said plurality of electrodes to produce a first image signal detected by said front zone and a second image signal detected by said back zone; and

producing an imaging signal from said first and second image signals.

22. The method of claim 21 wherein the gaseous medium is selected from the group consisting of argon, xenon, krypton, and mixtures thereof, and at least one of argon, xenon, krypton and their mixtures in combination with at least one of a polar and a quenching compounds.

23. The method of claim 22 wherein the gaseous medium is maintained at a predetermined pressure in a direct ionization mode to provide a high quantum efficiency and a reduced electron range.

24. The method of claim 21 further comprising the step of

applying an electric field between the detector cathode and said plurality of electrodes to produce said imaging signal.

25. The method of claim 24, further comprising the step of

providing an imaging system for receiving and processing said imaging signal.

26. The method of claim 25 wherein said step of exposing includes the step of imparting the incident radiation from a scanning beam geometry or an open beam geometry.

27. The method of claim 21, further comprising the step of

photolithographically disposing the plurality alternating anodes and cathodes on the substrate.

28. The method of claim 27, further comprising the steps of providing said substrate at least partially insulated and coupling one of a Kumakhov lens or a plurality of capillary optics with said substrate to provide an enhanced image.

29. The method of claim 21 further comprising the step of

providing a neutral zone between said front zone and said back zone, the neutral zone facilitating a distinction between the first and second image signals.

30. The method of claim 21 further comprising the steps of:

inserting a pre-filter between the incident radiation and the subject to produce a bimodal x-ray spectrum that is passed through the subject; and

directing the bimodal x-ray spectrum through a detector housing which carries a window through which the bimodal x-ray spectrum is passed, wherein the housing carries the substrate.

31. The method of claim 21, further comprising the step of

disposing the detector cathode between a radioactive plate source and the substrate to provide means for quantitative autoradiography.

32. The method of claim 31, further comprising the step of

emitting a predetermined level of radiation to ionize said gas detection medium.

33. The method of claim 21 further comprising the step of

inserting the substrate into a photo-tube filled with the gaseous medium to provide means for positron emission tomography gamma camera, computer tomography or single photon emission tomography.

34. The method of claim 33 further comprising the steps of

providing a primary detection region and a transfer gap within the photo-tube;

and

coupling a readout circuit to the phototube to generate the imaging signal.

35. The method of claim 34 further comprising the steps of

providing said primary detection region with a crystal for absorbing radiation from a radiation source adjacent the photo-tube, said radiation source generating a start signal received by said readout circuit;

generating scintillation light from the crystal for ionizing the gaseous medium which generates a plurality of photoelectrons;

multiplying said plurality of electrons in a preamplification grid to generate a signal received by said readout circuit; and

providing a mesh between said preamplification grid and said substrate to register a coincidence event and generate a stop pulse received by said readout circuit, wherein said detector generates a position reading and said readout circuit determines a difference between said start and stop pulses for association with said position reading.

36. The method of claim 21 further comprising the steps of

disposing a semiconductor substrate between the substrate and a plate, wherein a voltage is applied between the plate and said plurality of electrodes;

and

pressurizing said gas medium to a predetermined pressure.

37. The method claim 36 further comprising the steps of

imparting radiation from a scanning beam geometry;

and

producing electrons by direct x-ray ionization of the semiconductor substrate, wherein the electrons are drifted toward the first plurality of anode strips to generate the imaging signal.

38. The method of claim 21 further comprising the steps of

disposing a photosensitive coating over the substrate;

and

coupling the substrate to means for generating light that is exposed to the incident radiation.

39. The method of claim 38 further comprising the step of

providing a scintillation crystal carried by a window of a detector housing.

40. The method of claim 39 further comprising the steps of

providing a detector housing with a window which receives one of a scintillator crystal and a fiber optic plate, said housing also receiving said substrate;

and

disposing a photosensitive coating on a surface of one of said scintillator crystal or said fiber optic plate.

41. The method of claim 38 further comprising the step of

providing a plurality of scintillating fibers coupled to the photosensitive coating and carried in a detector housing.