Directional radiation detector and imager

• US 5,665,970 A
• Filed: 07/03/1996
• Issued: 09/09/1997
• Est. Priority Date: 07/03/1996
• Status: Expired due to Term

• Current Assignee: United States Department of the Army (Government of the United States of America)
• Original Assignee: The United States Of America As Represented By The Secretary Of The Army
• Inventors: Brucker, George J., Kronenberg, Stanley
• Primary Examiner(s): Glick, Edward J.
• Application Number:
  US08/687,095
• Time in Patent Office: 433 Days
• Field of Search: 250/336.1, 250/367, 250/366, 250/374, 250/370.1, 250/370.11, 250/390.11, 250/390.12, 250/370.01, 250/370.09, 250/361 R
• US Class Current: 250/374
• CPC Class Codes: G01T 1/18 with counting-tube arrangements, e.g. with Geiger counters tubes H01J47/08; with alarm provision G01T7/125

Abstract

A radiation sensor and/or imager is formed by sandwiching two materials having different atomic numbers (Z) around a radiation detector, such as scintilator or Geiger-Mueller type radiation counters, or solid state radiation detectors, such as those made of silicon). In one embodiment of the present invention, a thin layer of lead (Pb) is placed on one side of a Geiger-Mueller radiation counter and a layer of Lucite™ is disposed on the opposite side. One example, of a preferred Geiger-Mueller counter which may be used in the present invention is a modified pancake Geiger-Mueller counter with thin ruby mica windows, approximately 2.8 mg/cm² thick on both sides. By disposing a high Z material on one side of a radiation detector such as a Geiger-Mueller (GM) or a Scintillator Counter (SC) and a low Z material on an opposite side of either type of the counter, it is possible to detect the photo-Compton electrons emitted from the high or low Z material in the forward or backward directions and the attenuation of the emitted electrons by the high Z material. Because the Geiger-Mueller or scintillation counter can detect single events, the directional radiation detector according to the present invention can detect radiation intensities down to background radiation levels, which is approximately 0.15 μGy h^-1. Given the difference in the count rate (or intensity), the direction of the radiation source may be easily calculated by simply rotating the detector or by having two counters displaced in different angles (such as 180 degrees) so as to be able to take the difference of the number counts (or mirrors of the intensities).

Claims

1. A directional radiation detector comprising:

means sensitive to radiation having at least a first and second side;

a first region of material having a first atomic number and disposed on the first side of the means sensitive to radiation;

a second region of material having a second atomic number which is different from that of the atomic number of the first region of material and disposed on the second side of the means sensitive to radiation;

wherein the first and second atomic numbers of the first and second regions are sufficiently different such that when radiation is incident to the detector, there is a difference in forward and backward emissions of electrons between the first and second regions;

means to detect a signal from the means sensitive to radiation.

2. The detector of claim 1 further comprising means to rotate the detector.

3. The detector of claim 2 wherein the means sensitive to radiation is a Geiger Muller counter.

4. The detector of claim 3 wherein the Geiger Mueller counter has at least two sides which are permeable to radiation.

5. The detector of claim 4 wherein the at least two sides of the Geiger Mueller counter are thin.

6. The detector of claim 2 wherein the means sensitive to radiation is a scintillation counter.

7. The detector of claim 2 wherein the means sensitive to radiation is a solid state counter.

8. The detector of claim 2 wherein the first region of material is made of plastic and the second region of material is made of high atomic number material.

9. The detector of claim 2 further comprising means to calculate the direction of a maximum number of signals from the means to detect a signal.

10. A directional radiation detector comprising:

at least two means sensitive to radiation, each means having at least a first and second side;

at least two regions of material having a first atomic number and disposed on each of the first sides of the means sensitive to radiation;

at least two regions of material having a second atomic number which is different from that of the atomic number of the first region of material and disposed on each of the second sides of the means sensitive to radiation;

wherein the first and second atomic numbers of the first and second regions of each means sensitive to radiation are sufficiently different such that when radiation is incident to the detector, there is a difference in forward and backward emissions of electrons between the first and second regions;

means to detect a signal from the at least two means sensitive to radiation.

11. The detector of claim 10 further comprising means to rotate the detector.

12. The detector of claim 11 wherein the means sensitive to radiation is a Geiger Mueller counter.

13. The detector of claim 12 wherein the Geiger Mueller counter has at least two sides which are permeable to radiation.

14. The detector of claim 13 wherein the at least two sides of the Geiger Mueller counter are made of thin.

15. The detector of claim 11 wherein the means sensitive to radiation is a scintillation counter.

16. The detector of claim 11 wherein the means sensitive to radiation is a solid state counter.

17. The detector of claim 11 wherein the first region of material is made of plastic and the second region of material is made of a high atomic number material.

18. The detector of claim 11 further comprising means to calculate the direction of a maximum number of signals from the means to detect a signal.

19. A radiation imager comprising:

at least two means sensitive to radiation, each means having at least a first and second side;

at least two regions of material having a first atomic number and disposed on each of the first sides of the means sensitive to radiation;

at least two regions of material having a second atomic number which is different from that of the atomic number of the first region of material and disposed on each of the second sides of the means sensitive to radiation;

wherein the first and second atomic numbers of the first and second regions of each means sensitive to radiation are sufficiently different such that when radiation is incident to the detector, there is a difference in forward and backward emissions of electrons between the first and second regions;

means to detect a signal from the at least two means sensitive to radiation;

means to rotate the imager; and

means to calculate a first derivative of signals detected from the means to detect a signal and an angle of rotation of the imager.