Accelerating fissile material detection with a neutron source
View Patent ↗A neutron detector system for discriminating fissile material from non-fissile material wherein a digital data acquisition unit collects data at high rate, and in real-time processes large volumes of data directly to count neutrons from the unknown source and detecting excess grouped neutrons to identify fission in the unknown source. The system includes a Poisson neutron generator for in-beam interrogation of a possible fissile neutron source and a DC power supply that exhibits electrical ripple on the order of less than one part per million. Certain voltage multiplier circuits, such as Cockroft-Walton voltage multipliers, are used to enhance the effective of series resistor-inductor circuits components to reduce the ripple associated with traditional AC rectified, high voltage DC power supplies.
1. A method of characterizing neutrons, comprising:
receiving neutrons emitted from one or more neutron sources, wherein the emitted neutrons comprise at least one of: background neutrons from alpha-n reactions, cosmic-induced neutrons, and fission neutrons;
detecting the emitted neutrons in a first detector calibrated to a fast time scale having a scale on the order of nanoseconds to generate a first set of neutrons;
detecting the emitted neutrons also in a second detector calibrated to a slow time scale having a scale on the order of milliseconds to generate a second set of detected neutrons;
repeating a defined measurement time period for a defined number of times; and
analyzing the first and second set of detected neutrons to determine the number of times that a group of n simultaneously emitted neutrons is observed after the defined measurement time period is repeated the defined number of times to derive a neutron count measurement based on at least one of the fast time scale and the slow time scale to determine whether the emitted neutrons are fission neutrons.
2. The method of claim 1 wherein the background neutrons from alpha-n reactions feature a distribution having a first count distribution shape over a plurality of periods encompassing at least one of the fast time scale and the slow time scale;
the cosmic-induced neutrons have a second count distribution shape over a plurality of time periods encompassing the fast time scale; and
the fission neutrons are controlled by a relatively slow fission neutron speed and have a third count distribution shape over a plurality of periods encompassing the slow time scale.
3. The method of claim 1 wherein the first detector comprises a scintillator and energy selector system that is configured to detect fast and direct neutrons emitted from the one or more neutron sources.
4. The method of claim 3 wherein the second detector comprises at least one of a moderated neutron capture detector or scintillator-based detector configured to detect the emitted neutrons emitted in correspondence with the slow time scale.
5. The method of claim 1 further comprising:
generating neutrons in a neutron generator for detection by at least one of the first detector and the second detector, wherein the neutron generator is configured to induce fission in the one or more neutron sources;
subtracting an expected number of pairs of neutrons emitted by a hypothetical non-fission Poisson neutron source embodied in the neutron generator during a measurement time period from a number of pairs of observed neutrons derived from the neutron count measurement; and
characterizing the emitted neutrons as fission neutrons if the number of pairs of observed neutrons exceeds the expected number of pairs of neutrons in at least a portion of a histogram derived for the Poisson neutron source as compared to a histogram derived for the neutron count measurement.
6. The method of claim 5 wherein the first and second detectors are configured to distinguish between neutrons generated in the first neutron generator and induced neutrons emitted from the one or more neutron sources.
7. The method of claim 1 further comprising providing a Poisson neutron source in addition to the one or more neutron sources, for use in an in-beam interrogation system that imposes no perceptible electrical ripple to distort the correlation of generated neutrons.
8. The method of claim 7 wherein the Poisson neutron source comprises a compact 60 keV electric neutron source.
9. The method of claim 2 further comprising comparing a neutron correlation distribution shape of the emitted neutrons against a Poisson distribution, the second count distribution, and the third count distribution to determine whether or not the emitted neutrons are fission neutrons.