Neutron camera employing row and column summations

• US 9,366,769 B2
• Filed: 01/15/2013
• Issued: 06/14/2016
• Est. Priority Date: 01/31/2012
• Status: Active Grant

• Current Assignee: UT-Battelle LLC
• Original Assignee: UT-Battelle LLC
• Inventors: Clonts, Lloyd G., Diawara, Yacouba, Donahue, Cornelius Jr., Montcalm, Christopher A., Riedel, Richard A., Visscher, Theodore
• Primary Examiner(s): Sung, Christine
• Application Number:
  US14/376,018
• Publication Number:
  US 20140353511A1
• Time in Patent Office: 1,246 Days
• US Class Current: 1/1
• CPC Class Codes: G01T 3/06 with scintillation detectors

Abstract

For each photomultiplier tube in an Anger camera, an R×S array of preamplifiers is provided to detect electrons generated within the photomultiplier tube. The outputs of the preamplifiers are digitized to measure the magnitude of the signals from each preamplifier. For each photomultiplier tube, a corresponding summation circuitry including R row summation circuits and S column summation circuits numerically add the magnitudes of the signals from preamplifiers for each row and for each column to generate histograms. For a P×Q array of photomultiplier tubes, P×Q summation circuitries generate P×Q row histograms including R entries and P×Q column histograms including S entries. The total set of histograms include P×Q×(R+S) entries, which can be analyzed by a position calculation circuit to determine the locations of events (detection of a neutron).

Claims

1. A neutron camera comprising:

a scintillator plate;

at least one detector unit, wherein each of said at least one detector unit comprises;

a photomultiplier tube located on a back side of said scintillator plate and comprising an R×

S matrix of outputs, wherein R and S are integers greater than 1;

an R×

S array of preamplifiers configured to amplify each output from said R×

S matrix of outputs and to generate R×

S amplified signals; and

a signal conversion circuitry configured to generate a set of R row summation signals and a set of S column summation signals from said R×

S amplified signals; and

a position calculation unit configured to analyze a distribution of first time-integrated sums derived from said set of R row summation signals and a distribution of second time-integrated sums derived from said set of S column summation signals to identify an event location in said scintillator plate at which a neutron causes scintillation.

2. The neutron camera of claim 1, wherein said at least one detector unit is a P×

Q array of detector units, wherein P and Q are integers greater than 1.

3. The neutron camera of claim 2, wherein said distribution of first time-integrated sums includes P×

R first time-integrated sums, and said distribution of second time-integrated sums includes Q×

S second time-integrated sums.

4. The neutron camera of claim 3, wherein said position calculation unit is configured to fit said P×

R first time-integrated sums with a row fitting function and to identify a row coordinate of said event location, and to fit said Q×

S second time-integrated sums with a column fitting function and to identify a column coordinate of said event location.

5. The neutron camera of claim 4, wherein each of said row fitting function and said column fitting function has a functional form that strictly decreases with distance from a maximum value point.

6. The neutron camera of claim 5, wherein said functional form includes at least one term that is proportional to a Gaussian function.

7. The neutron camera of claim 4, wherein said fitting of said P×

R first time-integrated sums and said fitting of said Q×

S second time-integrated sums is performed employing a least square fitting method.

8. The neutron camera of claim 1, wherein each of said at least one signal conversion circuitry is embodied in a field programmable gate array (FPGA), and said position calculation unit is embodied in another field programmable gate array (FPGA).

9. The neutron camera of claim 1, wherein each of said R row summation signals is proportional to a sum of all amplified signals originating from a corresponding row within said R×

S matrix of outputs, and each of said S column summation signals is proportional to a sum of all amplified outputs originating from a corresponding column within said R×

S matrix of outputs.

10. The neutron camera of claim 9, wherein said detector unit further comprises R+S analog-to-digital (AD) converter circuits configured to convert said R row summation signals into R digitized row summation signals and said S column summation signals into S digitized column summation signals.

11. The neutron camera of claim 1, wherein said at least one detector unit further comprises a signal discrimination unit configured to trigger integration of said set of R row summation signals and said set of S column summation signals.

12. The neutron camera of claim 11, wherein said signal discrimination unit triggers said integration of signals if a parameter value generated from said set of R row summation signals and said set of S column summation signals exceeds a predefined threshold value.

13. A method of operating a neutron camera comprising:

providing a neutron camera including a scintillator plate and at least one detector unit, wherein each of said at least one detector unit comprises at least a photomultiplier tube located on a back side of said scintillator plate and comprising an R×

S matrix of outputs, and an R×

S array of preamplifiers configured to amplify each output from said R×

S matrix of outputs and to generate R×

S amplified signals, wherein R and S are integers greater than 1;

generating, for each of said at least one detector unit, a set of R row summation signals and a set of S column summation signals; and

determining an event location in said scintillator plate at which a neutron causes scintillation by analyzing a distribution of first time-integrated sums derived from said at least one set of R row summation signals and a distribution of second time-integrated sums derived from said at least one set of S column summation signals.

14. The method of claim 13, wherein said at least one detector unit is a P×

Q array of detector units, wherein P and Q are integers greater than 1.

15. The method of claim 13, wherein said determining of said event location comprises:

fitting said distribution of first time-integrated sums with a row fitting function and to identify a row coordinate of said event location; and

fitting said distribution of second time-integrated sums with a column fitting function and to identify a column coordinate of said event location.

16. The method of claim 15, wherein each of said row fitting function and said column fitting function has a functional form that strictly decreases with distance from a maximum value point.

17. The method of claim 13, wherein each of said R row summation signals is proportional to a sum of all amplified signals originating from a corresponding row within said R×

S matrix of outputs, and each of said S column summation signals is proportional to a sum of all amplified outputs originating from a corresponding column within said R×

S matrix of outputs.

18. The method of claim 17, further comprising:

converting each set of R row summation signals into a set of R digitized row summation signals; and

converting each set of S column summation signals into a set of S digitized column summation signals.

19. The method of claim 18, further comprising triggering integration of signals for said first and second time-integrated sums based on whether a parameter value generated from said at least one set of R row summation signals and said at least one set of S column summation signals exceeds a predefined threshold value.