IP Library Granted Patent US 11,079,504
Granted Patent B2
US 11,079,504 · App. 15/971,767 · Granted Aug 3, 2021

Differential neutron spectrum generator and related methods and systems

Inventor: Wade Scates (Idaho Falls, ID)
Assignee: Battelle Energy Alliance, LLC
G01T7/005G01T3/065G01T3/085G21G4/02H05H3/06
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Quick Facts
Patent No.
US 11,079,504
App. No.
15/971,767
Granted
Aug 3, 2021
Kind
B2
Abstract

A neutron spectrum generator is disclosed herein including a neutron source, a scatterer positioned in a direct path between the neutron source and a neutron detector, and a material shell configured to have at least one non-uniform characteristic selected from the group consisting of a material, a thickness, a length, an angle, a layer, and combinations thereof to generate a specific spectrum at the neutron detector that is different than the spectrum of the neutron source. A related method includes measuring a first response generated by a first material shell of a neutron spectrum generator interacting with a neutron source, replacing the first material shell with a second material shell, measuring a second response generated by a second material shell of a neutron spectrum generator interacting with the neutron source, and determining a total fission response by determining a difference between the first response and the second response.

Claims (27)

1. A neutron spectrum generator, comprising:

a neutron source;

a scatterer positioned in a direct path between the neutron source and a neutron detector; and

at least one material shell positioned proximate the neutron source, and configured with at least one non-uniform characteristic selected from the group consisting of a material, a thickness, a length, an angle, a layer, and combinations thereof to generate a specific spectrum responsive to interacting with neutrons that is different than a spectrum of the neutron source.

2. The neutron spectrum generator of claim 1 , wherein the at least one material shell is a cylindrical shape.

3. The neutron spectrum generator of claim 1 , wherein the at least one material shell is a hemispheric shape.

4. The neutron spectrum generator of claim 1 , wherein the at least one material shell is a shape symmetric about its axis, wherein the axis is a vector extending from the neutron source through the scatterer to the neutron detector.

5. The neutron spectrum generator of claim 1 , wherein the at least one non-uniform characteristic of the material shell is divided according to angular wedges of the material shell.

6. The neutron spectrum generator of claim 1 , wherein the neutron source is a DT generator configured to produce neutrons by fusion of deuterium (D) and tritium (T).

7. The neutron spectrum generator of claim 1 , wherein the neutron source is a DD generator configured to produce neutrons by fusion of deuterium (D) and deuterium (D).

8. The neutron spectrum generator of claim 1 , wherein the neutron source is selected from the group consisting of a gamma source configured to eject a neutron, an electron accelerator beam, and a Bremsstrahlung converter.

9. The neutron spectrum generator of claim 1 , wherein the at least one material shell includes multiple material shells.

10. The neutron spectrum generator of claim 9 , wherein the multiple material shells are configured to generate the specific spectrum exhibiting multiple peaks.

11. The neutron spectrum generator of claim 1 , wherein the specific spectrum is an approximation of the spectrum for Californium-252, and the neutron source is a different source than Californium-252.

12. A method for generating a specific neutron spectrum, the method comprising:

measuring a first response generated responsive to a first material shell of a neutron spectrum generator interacting with a neutron source;

replacing the first material shell with a second material shell;

measuring a second response generated responsive to the second material shell of a neutron spectrum generator interacting with the neutron source; and

determining a total fission response by determining a difference between the first response and the second response.

13. The method of claim 12 , further comprising forming the first material shell and the second material shell to each have at least one non-uniform characteristic selected from the group consisting of a material, a thickness, a length, an angle, a layer, and combinations thereof to generate a specific spectrum at a neutron detector that is different than a spectrum of the neutron source.

14. The method of claim 13 , further comprising forming the first material shell and the second material shell to each have a cylindrical shape.

15. The method of claim 12 , further comprising forming the first material shell including uranium and the second material shell including lead.

16. The method of claim 12 , further comprising generating neutrons with the neutron source.

17. The method of claim 16 , wherein generating neutrons with the neutron source includes utilizing at least one of a DT generator, a DD generator, a gamma source configured to eject a neutron, an electron accelerator beam, or a Bremsstrahlung converter.

18. The method of claim 12 , wherein measuring the first response and the second response each include utilizing an active neutron detector.

19. The method of claim 12 , wherein measuring the first response and the second response each include utilizing a passive neutron detector.

20. The method of claim 12 , wherein measuring the first response and measuring the second response comprises measuring one of the first response and the second response as a positive response and the other of the first response and the second response as a negative response.

Assignments (2)
CONFIRMATORY LICENSE Recorded Sep 10, 2018
From: BATTELLE ENERGY ALLIANCE/IDAHO NAT'L LAB
To: UNITED STATES DEPARTMENT OF ENERGY
Reel/Frame 047036/0643 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 7, 2018
From: SCATES, WADE
To: BATTELLE ENERGY ALLIANCE, LLC
Reel/Frame 045730/0438 →
Continuity (2)
Provisional Application 62505200 · May 12, 2017
Related Publication 20180329091A1 · Nov 15, 2018