Detection of special nuclear material and other contraband by prompt and/or delayed signatures from photofission

1. A method of examining contents of an object, the method comprising:

injecting a plurality of radiofrequency power pulses into an accelerator, the plurality of radiofrequency power pulses being separated by first gaps;

injecting a plurality of charged particle pulses into the accelerator while each of the plurality of radiofrequency pulses are injected into the accelerator, the plurality of charged particle pulses being separated by second gaps smaller than the first gaps;

impacting a target material by each of the plurality of accelerated charged particles to generate macropulses of radiation corresponding to each radiofrequency pulse, each macropulse being separated by the first gaps and containing a plurality of micropulses of radiation corresponding to the plurality of charged particles injected into the accelerator during each radiofrequency power pulse;

scanning an object by the plurality of consecutive macropulses of radiation comprising the respective pluralities of consecutive micropulses of radiation;

checking for prompt gamma rays detected in respective first time periods in respective second gaps between respective consecutive micropulses of radiation and not during any of the respective consecutive micropulses, the respective first time periods being based, at least in part, on respective expected arrival times of prompt gamma rays at a first detector resulting from photofission within the object, if any, induced by a respective consecutive micropulse;

checking for prompt neutrons detected in respective second time periods in respective second gaps between respective consecutive micropulses of radiation and not during any of the respective consecutive micropulses, the respective second time periods being based, at least in part, on respective expected arrival times of prompt neutrons at a second detector resulting from photofission within the object, if any, induced by a respective consecutive micropulse;

checking for delayed gamma rays detected in respective third time periods in respective first gaps between respective consecutive macropulses of radiation and not during either of the respective consecutive macropulses, the respective third time periods being based, at least in part, on respective expected arrival times of delayed gamma rays at the first detector resulting from photofission within the object, if any, induced by a respective consecutive macropulse;

checking for delayed neutrons detected in respective fourth time periods in respective first gaps between respective consecutive macropulses of radiation and not during any of the respective consecutive macropulses, the respective fourth time periods being based, at least in part, on respective expected arrival times of delayed neutrons at the second detector resulting from photofission within the object, if any, induced by the respective consecutive macropulse; and

determining whether the object at least potentially contains Special Nuclear Material based, at least in part, on the checks for the detection of the prompt gamma rays, prompt neutrons, delayed gamma rays, and/or delayed neutrons.

2. The method of claim 1 , wherein:

the charged particle pulses are separated by from about 100 nanoseconds to about 300 nanoseconds; and

the charged particle pulses are from about 0.5 nanoseconds to about 10 nanoseconds long.

3. The method of claim 1 , wherein:

the first detector is a first distance from the object;

the second detector is a second distance from the object;

a source of the first and second radiation pulses is a third distance from the object;

the first expected arrival time is based, at least in part, on the first and third distances; and

the second expected arrival time is based, at least in part, on the second and third distances.

4. The method of claim 1 , wherein the micropulses and macropulses of radiation comprise X-ray radiation.

5. The method of claim 4 , further comprising:

scanning the object by consecutive neutrons pulses;

checking for the detection of prompt and/or delayed gamma rays resulting from scanning by the neutron pulses;

checking for the detection of prompt and/or delayed neutrons resulting from scanning by the neutron pulses; and

further determining whether the object at least potentially contains explosives, drugs, chemical agents, and/or biological agents based, at least in part, on the check for the detection of the gamma rays and the check for the detection of neutrons resulting from the scanning by the consecutive neutron pulses.

6. The method of claim 5 , further comprising:

determining an identity of contents of the object based, at least in part, on the check for the detection of gamma rays and the check for the detection of neutrons resulting from scanning by the neutron pulses.

7. The method of claim 1 , further comprising:

detecting consecutive radiation pulses transmitted through the object;

generating a transmission image based on detected consecutive radiation pulses; and

determining whether the object at least potentially comprises Special Nuclear Material based, at least in part, on the spatial image.

8. The method of claim 1 , further comprising:

determining a location of the at least potential Special Nuclear Material in the object based, at least in part, on respective detection times for the prompt gamma rays, prompt neutrons, delayed gamma rays, and/or delayed neutrons at the first and second detectors.

9. The method of claim 1 , comprising:

determining, by a processor, that the object at least potentially contains Special Nuclear Material if both prompt gamma rays and prompt neutrons are detected; and

confirming, by the processor, that the object contains Special Nuclear Material if at least one of delayed gamma rays and delayed neutrons are detected.

10. The method of claim 1 , comprising detecting prompt gamma rays, prompt neutrons, delayed gamma rays, delayed neutrons by the same detector.

11. The method of claim 1 , wherein the delayed gamma rays and the delayed neutrons are produced microseconds to hundreds of milliseconds after emission of the prompt gamma rays and the prompt neutrons.

12. The method of claim 11 , wherein the prompt gamma rays and the prompt neutrons are produced on the order of 10 −15 -10 −12 seconds after photofission.

13. The method of claim 1 , wherein the prompt gamma rays and the prompt neutrons are produced on the order of 10 −15 -10 −12 seconds after photofission.

14. The method of claim 1 , comprising scanning the object by a pattern of macropulses comprising micropulses.

15. The method of claim 1 , further comprising, after scanning:

detecting at least one of prompt gamma rays, prompt neutrons, delayed gamma rays, and delayed neutrons.

16. The method of claim 15 , comprising:

checking for the detection of prompt gamma rays and delayed gamma rays by at least one first detector positioned to detect prompt gamma rays and delayed gamma rays; and

checking for the detection of prompt neutrons and delayed neutrons by at least one second detector positioned to detect prompt neutrons and delayed neutrons; and

the method further comprising:

gating the at least one first detector to a high gain during the first time periods to detect the prompt gamma rays;

gating the at least one second detector to a high gain during the second time periods to detect the prompt neutrons;

gating the at least one first detector to a high gain during the third time periods to detect the delayed gamma rays; and

gating the at least one second detector to a high gain during the fourth time periods to detect the delayed neutrons.

17. The method of claim 16 , wherein the at least one first detector and the at least one second detector are the same.