Method and apparatus for the identification of lithospheric or shielded material deposits by doppler-shifted response photon spectra from interrogation by ionizing radiation

• US 8,193,504 B2
• Filed: 04/22/2009
• Issued: 06/05/2012
• Est. Priority Date: 05/03/2008
• Status: Active Grant

• Current Assignee: Luca Joseph Gratton
• Original Assignee: Luca Joseph Gratton
• Inventors: Gratton, Luca Joseph
• Primary Examiner(s): Hannaher, Constantine
• Application Number:
  US12/386,803
• Publication Number:
  US 20090272906A1
• Time in Patent Office: 1,140 Days
• Field of Search: 376/159, 250/358.1
• US Class Current: 250/358.1
• CPC Class Codes: G01T 3/00 Measuring neutron radiation G01T5/00 takes precedence
• CPC Class Codes: G01V 5/20 Detecting prohibited goods, e.g. weapons, explosives, hazardous substances, contraband or smuggled objects
• CPC Class Codes: G01V 5/234 Measuring induced radiation, e.g. thermal neutron activation analysis

Abstract

A method and apparatus for the remote, non-invasive detection or characterization of materials manifests a controlled temperature perturbation to the sample material location concurrently with sample interrogation by ionizing radiation and with detection of the response emission energy spectra. This configuration induces and detects Doppler effects manifested at the sample location, allowing material inventory and composition measurements, and allowing a comparative reduction of the exposure duration compared to other isothermal proportional count, coincidence count or spectral analysis techniques. The method and apparatus apply primarily to the detection of elements and isotopes in baggage handling, cargo inspection, chemical characterization, process control and geologic operations, though the method and apparatus are not restricted to these applications. Though the magnitudes of the measured effects are substance specific, the contributing physical processes are not strictly material dependent, allowing method and apparatus applications to almost any high-energy photon-emitting material in multiple applications.

Claims

1. A method for the remote detection and characterization of materials at a sample material emplacement with ionizing radiation, that requires thermally-induced Doppler broadening of nuclear reaction cross sections, comprising the steps of:

(a) generating a unidirectional interrogation beam composed of ionizing radiation at a platform used as a stage for a detection and characterization operation;

(b) directing an interrogation beam composed of ionizing radiation to irradiate a remote sample material emplacement or a portion thereof;

(c) generating a secondary ionizing photon radiation by spontaneous, particle capture, inelastic particle scattering, and particle activation reactions of the interrogation beam with the material at the emplacement location;

(d) detecting secondary photon radiations emitted from the sample material emplacement in interaction events in detector materials disposed at a remote location adjacent to the location where the interrogation beam originates;

(e) converting interaction events by secondary photons, including those emitted from the sample material emplacement location, with the detector materials to detector response electronic signals;

(f) processing the detector response electronic signals remotely to generate spectral information by cataloging the actuarial detection frequency or cumulative event count in specific incident photon energy intervals;

(g) changing the temperature of the sample material emplacement remotely in a controlled fashion to induce Doppler broadening of nuclear reaction cross sections by use of an apparatus disposed for the purpose of creating said temperature change;

(h) and, assessing remotely the changes produced by sample material emplacement temperature perturbations to the spectral information generated from the detector response electronic signals to calculate or infer the mass inventory and composition of material at the sample emplacement.

2. A method according to claim 1, wherein an interrogation beam composed of ionizing radiation comprises neutron radiation directed to irradiate the sample material emplacement or a portion thereof.

3. A method as in claim 1, wherein an interrogation beam composed of ionizing radiation comprises photon radiation directed to irradiate the sample material emplacement or a portion thereof.

4. A method as in claim 3, wherein a secondary ionizing photon radiation occurs by capture, inelastic scatter, spontaneous, or photo-nuclear reactions of an interrogation photon beam with the material at the emplacement location.

5. An apparatus for the remote detection and characterization of materials at a sample material emplacement with ionizing radiation, that manifests thermally-induced Doppler broadening of nuclear reaction cross sections, with said apparatus comprising:

(a) an ionizing radiation source having a beam controller and collimator that collectively operate to provide a unidirectional interrogation beam of selected energy that can be operated in pulsed or continuous modes;

(b) a transportable platform that bears the ionizing radiation source and beam controller, and allows directional adjustment of the emitted interrogation beam to aim said beam towards the sample material emplacement;

(c) a measurement detector array disposed on the platform to intercept photons generated at the sample emplacement location;

(d) a diagnostic detection system composed of multiple neutron detectors disposed on the platform to gauge interrogation source operation and radiation status;

(e) a signal processor and analyzer system that communicates with the measurement and diagnostic detectors to receive the detector output signals, process said signals to generate both system status, and spectral information by cataloging the actuarial detection frequency or cumulative event count in specific incident photon and neutron energy intervals, and to compare and manipulate said spectra in manners specified by the user for the purpose of system-keeping, sample material inventory and composition measurement;

(f) a thermal perturbation system, at least partially comprising an interrogation beam composed of ionizing radiation generated by the ionizing radiation source, that induces material temperature changes at the sample emplacement in a controlled and measured fashion;

(g) a thermal management system disposed on the platform for the purpose of stabilizing temperatures of detectors and other sensitive components;

(h) a transmitter/receiver system disposed on the platform and capable of operational command and data transfer communications;

(i) power cabling for the provision of externally supplied electrical power to electrically energized components disposed on the platform;

(j) a central controller system disposed on the platform that regulates, starts, stops and implements operational setpoints for the interrogation beam, diagnostic detector system, measurement detector system, thermal perturbation system, thermal management system and transmitter/receiver system;

(k) radiation shielding disposed on the platform to screen radiation-sensitive components;

(l) and, cabling for electrical connectivity among components disposed on the platform.

6. An apparatus according to claim 5, wherein the ionizing radiation source is a neutron source having a neutron beam controller and collimator that operates to provide a unidirectional interrogation neutron beam of selected energy that can be operated in pulsed or continuous modes.

7. An apparatus as in claim 6, wherein the neutron source is a D-T neutron generator.

8. An apparatus as in claim 6, wherein the neutron source is an encapsulated isotopic neutron emitter.

9. An apparatus as in claim 6, wherein the neutron source is an encapsulated isotopic alpha emitter embedded in neutron-generating matrix material.

10. An apparatus as in claim 6, wherein the neutron source is an encapsulated isotopic photoneutron source.

11. An apparatus as in claim 6, wherein the neutron source is an electron beam accelerator with a neutron-generating target.

12. An apparatus as in claim 6, wherein the neutron source is fitted with a beam chopper-plate device.

13. An apparatus as in claim 6, wherein the dedicated component or system of components in the thermal perturbation system that induces the thermal perturbation to the sample material at the emplacement is exclusively the interrogation neutron beam generated by a neutron source.

14. An apparatus as in claim 5, wherein the ionizing radiation source is an ionizing photon source having a photon beam controller that operates to provide a unidirectional interrogation photon beam of selected energy that can be operated in pulsed or continuous modes.

15. An apparatus as in claim 14, wherein an ionizing photon source having a photon beam controller is disposed in the form of an electron accelerator fitted with a photon-generating converter material and beam diverter.

16. An apparatus as in claim 14, wherein the dedicated component or system of components in the thermal perturbation system that induces the thermal perturbation to the sample material at the emplacement is exclusively the interrogation photon beam generated by a photon source.

17. An apparatus as in claim 5, wherein the measurement detectors are arranged in a common plane as a monolithic structure with a cavity at the center comprising a beam port.

18. An apparatus as in claim 5, wherein the measurement detectors are arranged in a common plane as a monolithic structure capable of orientation adjustments on two perpendicular axes residing in the plane of the detector array for the purpose of aiming the apparatus.

19. An apparatus as in claim 5, wherein the measurement detector array comprises component detectors containing active semiconductor materials.

20. An apparatus as in claim 5, wherein the measurement detector array comprises high-purity Germanium detectors.

21. An apparatus as in claim 5, wherein the measurement detector array comprises component detectors containing active scintillation materials.

22. An apparatus as in claim 5, wherein the measurement detector array comprises Sodium Iodide detectors.

23. An apparatus as in claim 5, wherein the diagnostic detector system comprises a combination of Helium-3 and Helium-4 pressurized gas detectors.

24. An apparatus as in claim 5, wherein the central controller system is a programmable microprocessor.

25. An apparatus as in claim 5, wherein Polyethylene shielding is disposed.

26. An apparatus as in claim 5, wherein Lead shielding is disposed.

27. An apparatus as in claim 5, wherein Tungsten shielding is disposed.

28. An apparatus as in claim 5, wherein the thermal management system comprises distributed thermocouples, distributed evaporators, a programmable controller, distributed actuators, a vapor compression and heat rejection unit, refrigerant ducting, and Argon refrigerant.

29. An apparatus as in claim 5, wherein the thermal management system comprises distributed thermocouples, distributed evaporators, a programmable controller, distributed actuators, a vapor compression and heat rejection unit, refrigerant ducting, and Nitrogen refrigerant.

30. An apparatus as in claim 5, wherein the thermal management system comprises distributed thermocouples, distributed evaporators, a programmable controller, distributed actuators, a vapor compression and heat rejection unit, refrigerant ducting, and Carbon Dioxide refrigerant.

31. An apparatus as in claim 5, wherein the thermal management system comprises distributed thermocouples, distributed actuators, a power supply, electric wire leads, and distributed solid-state electronic cooling pads.

32. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is an ultrasonic acoustic generator.

33. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is a sonic acoustic generator.

34. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is a shock-tube or pressure generator.

35. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is a microwave generator.

36. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is a visible wavelength laser generator.

37. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is an infrared wavelength laser generator.

38. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is an electrical resistance heating device consisting of a current or voltage generator, electrical cable leads, electrodes, and the use of the sample emplacement material region as an effective electrical resistance element.

39. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is an electromagnetic induction device consisting of a current generator, a conductive induction winding that enshrouds the emplacement location, and the use of the sample and the material surrounding the emplacement as the inductor core plug material.

40. An apparatus as in claim 5, wherein the dedicated component or system of components in the thermal perturbation system that primarily induces the thermal perturbation to the sample material at the emplacement is a spatial heating device or fluid in direct contact with the sample material at the emplacement location.