Neutron detector

• US 7,923,698 B2
• Filed: 09/30/2009
• Issued: 04/12/2011
• Est. Priority Date: 06/19/2007
• Status: Expired due to Fees

• Current Assignee: Materials Innovation Incorporated, UT-Battelle LLC
• Original Assignee: Materials Innovation Incorporated, UT-Battelle LLC
• Inventors: Kisner, Roger A., Stephan, Andrew C., Jardret, Vincent D.
• Primary Examiner(s): Porta; David P
• Assistant Examiner(s): Kim; Kiho
• Application Number:
  US12/586,949
• Publication Number:
  US 20100155617A1
• Time in Patent Office: 559 Days
• Field of Search: 25039001-39012
• US Class Current: 250/390.01
• CPC Class Codes: G01T 1/00 Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation G01T3/00, G01T5/00 take precedence
• 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
• CPC Class Codes: Y10T 29/49117 Conductor or circuit manufacturing

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 on the outside of said dielectric body to create an electric field across said gas volume, where the peak voltage drop across said interior volume of said hollow dielectric body is at least 70% of the bias voltage applied between said electrodes, so that an electrical pulse may 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 2 wherein the ratio of said a wall thickness to said outside diameter of said hollow dielectric body is between 0.02 and 0.2.

4. The apparatus of claim 2 wherein said dielectric body has an outside diameter between 5 and 12 mm and a wall thickness between 0.05 and 0.4 mm.

5. The apparatus of claim 2 wherein the product of the diameter of said dielectric body and the density of the gas contained within said dielectric body (the areal density) is between 1.29×

10<sup>−

4</sup> and 1.07 g/cm².

6. The apparatus of claim 1 wherein said dielectric body has a bulk resistivity between 10⁹ and 10¹³ Ω

-m.

7. The apparatus of claim 1 wherein said dielectric body has a bulk resistivity around 2×

10¹¹ Ω

-m.

8. The apparatus of claim 1 wherein said maximum voltage drop across said interior volume of the dielectric body is at least 90% of said bias voltage.

9. 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.

10. 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.

11. An apparatus for detecting neutrons comprising:

a plurality of neutron sensors comprising hollow dielectric bodies having a bulk resistivity in the range from about 10⁸ to about 10¹⁷ Ω

-m, said dielectric bodies filled to a selected pressure with a gas capable of at least partial ionization by a neutron;

electrodes disposed on the external surfaces of said dielectric bodies and configured to establish an electric field within the interior volumes of said dielectric bodies, where the peak voltage drop across the interior volume of each of said sensors is at least 70% of the bias voltage applied between the electrodes, so that an electrical pulse may be collected in response to said ionization produced by an interaction of said neutron;

a volume of moderator material in which said neutron sensors are placed, said moderator material having a front surface, wherein some of said neutron sensors are placed closer to said front surface than are others; and

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

12. The apparatus of claim 11 wherein said hollow dielectric bodies comprise generally spherical sealed glass capsules having an outside diameter between about 0.1 and 30 mm and a wall thickness between about 10 μ

m and 5 mm.

13. The apparatus of claim 12 wherein the ratio of said a wall thickness to said outside diameter of said hollow dielectric body is between 0.02 and 0.2.

14. The apparatus of claim 11 wherein the product of the size of said dielectric bodies in at least one dimension and the density of the gas contained within said dielectric bodies (the areal density) is between 1.29×

10<sup>−

4</sup> and 1.07 g/cm².

15. The apparatus of claim 11 wherein at least some of said hollow dielectric bodies are individually addressable by said electrodes.

16. The apparatus of claim 11 wherein at least some of said hollow dielectric bodies may be addressed in parallel by said electrodes.

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

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/cmHg;

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

m to about 5 mm, wherein the ratio of said wall thickness to said interior dimension is between 0.02 and 0.2;

filling said body with a gas composition at a selected pressure, said gas composition capable of at least partial ionization by a neutron;

sealing said body to retain said gas; and

,

applying two electrodes on opposite sides, respectively, of said hollow glass body, said electrodes configured to apply a selected bias voltage to said hollow glass body, wherein the peak voltage drop across said selected interior dimension of said hollow body is at least 70% of said selected bias voltage.

18. The method of claim 17 further comprising the step of:

placing a plurality of said electroded hollow glass bodies within a volume of moderator material.

19. The method of claim 18 wherein said moderator material has a front surface, and some of said electroded hollow glass bodies are placed closer to said front surface than are others.

20. The method of claim 18 wherein at least some of said plurality of electroded hollow glass bodies may be individually addressable by said electrodes.