Neutron detector

• US 20080315108A1
• Filed: 06/19/2007
• Published: 12/25/2008
• Est. Priority Date: 06/19/2007
• Status: Abandoned Application

• Current Assignee: Materials Innovation Incorporated, UT-Battelle LLC
• Original Assignee: Materials Innovation Incorporated
• Inventors: Stephan, Andrew C., Kisner, Roger A., Jardret, Vincent D.
• Application Number:
  US11/820,261
• Publication Number:
  US 20080315108A1
• Time in Patent Office: Days
• US Class Current: 250/390.01
• CPC Class Codes: G01T 3/008 using an ionisation chamber filled with a gas, liquid or solid, e.g. frozen liquid, dielectric G01T3/006 takes precedence
• CPC Class Codes: H01J 47/1255 Ionisation chambers

Abstract

A neutron detector comprises a gas-filled dielectric shell, preferably a glass balloon, having opposite electrodes. An electric field is established whereby ionizing particles may be detected via ionization and current flow in the gas, using a pulse height analyzer or other conventional means. The dielectric shell preferably has low gas permeability and a bulk resistivity in the range of 10⁸ to 10¹⁷ Ω-m, and is preferably in the millimeter to centimeter size range. Multiple balloons may be arranged in parallel or may be individually addressable by the detector electronics.

Claims

1. An apparatus for detecting neutrons comprising:

a hollow dielectric body having a bulk resistivity in the range from about 10⁸ to about 10¹⁷ Ω

-m, said body containing an interior volume of gas capable of at least partial ionization by a neutron;

two electrodes in contact respectively with opposite sides of said dielectric body, said electrodes configured to create an electric field across said gas volume, whereby an electrical pulse will be detectable by said electrodes when an ionization event occurs within said interior volume; and

,

a detection circuit connected to said electrodes, said detection circuit capable of detecting said electrical pulse.

2. The apparatus of claim 1 wherein said dielectric body comprises a generally spherical sealed glass capsule having an outside diameter between about 0.1 and 30 mm and a wall thickness between about 10 μ

m and 5 mm.

3. The apparatus of claim 1 wherein said electric field is below the field necessary to cause operation in a Geiger-Mueller mode and said electric field is sufficient to detect ionization events in a mode selected from the following group:

ionization mode;

proportionality mode; and

limited proportionality mode.

4. The apparatus of claim 3 wherein said electric field is in the range from about 10 to 2000 V/cm.

5. The apparatus of claim 1 wherein said gas comprises a species selected from the following group:

H;

He;

³He;

Ne;

Ar;

C;

B;

Li;

Gd;

Th;

Pu; and

U.

6. The apparatus of claim 1 wherein said electrodes are selected from the group consisting of:

thin film metallizations;

thick film metallizations;

conductive polymers;

conductive paints;

flexible metal sheets;

metallized dielectric sheets; and

printed circuit boards.

7. The apparatus of claim 1 wherein said detection circuit contains at least one component selected from the following group:

pulse height analyzers;

pulse detectors;

multichannel analyzers;

linear amplifiers;

lower level discriminators;

pulse shape discriminators;

timing circuits; and

counters.

8. The apparatus of claim 1 wherein said dielectric comprises a glass having a gas permeability constant for helium at room temperature of less than 7.6×

10<sup>−

11</sup> cm³/sec/cm²/mm/cm·

Hg.

9. An apparatus for detecting neutrons comprising:

a substantially planar array of hollow dielectric shells, said shells filled with a gas capable of at least partial ionization by a neutron;

electrodes disposed on opposite sides of said planar array in electrical contact with said hollow dielectric shells whereby an electrical pulse may be collected in response to the passage of said neutron; and

,

a detection circuit connected to said electrodes, said detection circuit capable of detecting said electrical pulse.

10. The apparatus of claim 9 wherein at least some of said dielectric shells are individually addressable by said electrodes.

11. The apparatus of claim 9 wherein at least some of said dielectric shells may be addressed in parallel by said electrodes.

12. A method of making a neutron detector comprising the steps of:

a. formulating a glass composition having a bulk resistivity in the range of 10⁸ to 10¹⁷ Ω

-m and a gas permeability constant for helium at room temperature of less than 7.6×

10<sup>−

11</sup> cm³/sec/cm²/mm/cm·

Hg;

b. forming said glass into a hollow body having an interior dimension from about 0.1 to about 30 mm and a wall thickness from about 10 μ

m to about 5 mm;

c. filling said body with a gas composition capable of at least partial ionization by a neutron;

d. sealing said body to retain said gas; and

,

e. applying two electrodes on opposite sides, respectively, of said body.

13. The method of claim 12 wherein said gas comprises a species selected from the following group:

H;

He;

³He;

Ne;

Ar;

C;

B;

Li;

Gd;

Th;

Pu; and

U.

14. The method of claim 12 wherein said electrodes are selected from the group consisting of:

thin film metallizations;

thick film metallizations;

conductive polymers;

conductive paints;

flexible metal sheets;

metallized dielectric sheets; and

printed circuit boards.

15. The method of claim 12 wherein said gas has a pressure between about 1 and 200 atm.

16. The method of claim 12 further comprising the step of:

f. connecting said electrodes to a detection circuit.

17. The method of claim 16 wherein said detection circuit contains at least one component selected from the following group:

pulse height analyzers;

pulse detectors;

multichannel analyzers;

linear amplifiers;

lower level discriminators;

pulse shape discriminators;

timing circuits; and

counters.

18. An apparatus for detecting neutrons comprising:

a hollow dielectric body having a bulk resistivity in the range from about 10⁸ to about 10¹⁷ Ω

-m, said body containing an interior volume of gas capable of at least partial ionization by a neutron;

two electrodes disposed respectively on opposite sides of said dielectric body, said electrodes configured to create an electric field across said gas volume, said electric field being less than the field necessary to cause operation in a Geiger-Mueller mode, whereby an electrical pulse will be detectable by said electrodes when an ionization event occurs within said interior volume; and

,

a detection circuit connected to said electrodes, said detection circuit capable of detecting said electrical pulse.

19. The apparatus of claim 18 wherein said electric field is sufficient to detect ionization events in a mode selected from the following group:

ionization mode;

proportionality mode; and

limited proportionality mode.

20. The apparatus of claim 18 wherein said detection circuit contains at least one component selected from the following group:

pulse height analyzers;

pulse detectors;

multichannel analyzers;

linear amplifiers;

lower level discriminators;

pulse shape discriminators;

timing circuits; and

counters.