Active remote detection of radioactivity based on electromagnetic signatures

Patent metadata

Field	Value
Publication number	US-9835761-B2
Application number	US-201514599030-A
Country	US
Kind code	B2
Filing date	Jan 16, 2015
Priority date	Feb 5, 2014
Publication date	Dec 5, 2017
Grant date	Dec 5, 2017

Abstract

A system for the active remote detection of radioactivity from a target of interest includes a first laser source for generating an ionizing laser beam when remotely directed on a radioactive target of interest, a second laser source for generating a laser probe beam on the radioactive target of interest, and a spectrometer configured to measure the frequency modulation of the probe beam caused by the ionization from the radioactive target of interest.

First claim

What is claimed as new and desired to be protected by Letters Patent of the United States is:

1. A method for active remote detection of radioactivity from a radioactive target of interest that emits radiation causing ions to form in air surrounding the radioactive target of interest, the method comprising:
generating a laser beam using a first laser source, wherein the laser beam is configured to photo-detach the ions formed by the radioactive target of interest;
generating a laser probe beam using a second laser source;
directing the laser beam and the laser probe beam onto the radioactive target of interest;
measuring, based on a time evolution of electron density near the radioactive target of interest, a frequency modulation of the laser probe beam;
determining, based on the frequency modulation, an electromagnetic signature of the radioactive target of interest; and
identifying, based on the electromagnetic signature, a type of radioactive material in the radioactive target of interest.

2. The method of claim 1 , wherein the first laser source has a peak intensity of I peak =160 GW/cm 2 and a pulse duration of τ laser =1 nsec.

3. The method of claim 1 , wherein the laser probe beam has a frequency in the range of 90 GHz to 110 GHz.

4. The method of claim 1 , wherein identifying the type of radioactive material in the radioactive target of interest further comprises:
detecting a generation of a spark/air breakdown initiated by the laser beam.

5. The method of claim 1 , wherein the laser beam initiates an avalanche ionization in air surrounding the radioactive target of interest.

6. The method of claim 5 , wherein the avalanche ionization initiates an increase in electron density in the air surrounding the radioactive target of interest.

7. The method of claim 6 , wherein the increase in electron density induces the frequency modulation.

8. The method of claim 1 , wherein the measured frequency modulation corresponds to an increase in the electron density over time.

9. A system for the active remote detection of radioactivity from a radioactive target of interest, the system comprising:
a first laser source configured to generate a laser beam, wherein the laser beam is configured to photo-detach ions formed by the radioactive target of interest;
a second laser source configured to generate a laser probe beam directed on the radioactive target of interest; and
a spectrometer configured to measure, based on a time evolution of electron density near the radioactive target of interest, a frequency modulation of the laser probe beam caused by an increase in the electron density, initiated by the laser beam, in air surrounding the radioactive target of interest.

10. The system of claim 9 , wherein a radioactive composition of the radioactive target of interest is determined by:
measuring a frequency modulation of the laser probe beam,
determining, based on the frequency modulation, an electromagnetic signature of the radioactive target of interest, and
identifying, based on the electromagnetic signature, the radioactive target of interest as having a specific type of radioactive material.

11. The system of claim 9 , wherein the first laser source has a peak intensity of I peak =160 GW/cm 2 and a pulse duration of τ laser =1 nsec.

12. The system of claim 9 , wherein the laser probe beam has a frequency in the range of 90 GHz to 110 GHz.

13. The system of claim 9 , wherein the laser beam is configured to initiate an avalanche ionization in the air surrounding the radioactive target of interest.

14. The system of claim 13 , wherein the avalanche ionization initiates the increase in electron density.

15. The system of claim 14 , wherein the frequency modulation of the laser probe beam correlates to a type of radioactive material.

16. The system of claim 9 , wherein the spectrometer is configured to detect frequencies in the range of +/−10% of a frequency of the laser probe beam.

17. The system of claim 9 , wherein the spectrometer is further configured to:
detect a generation of a spark/air breakdown initiated by the laser beam.

18. A system for the active remote detection of radioactivity from a radioactive source that emits gamma rays causing O 2 − ions to form in air surrounding the radioactive source, the system comprising:
a first laser source configured to generate a laser beam, wherein the laser beam has a peak intensity and a pulse duration sufficient to photo-detach electrons from the O 2 − ions and initiate avalanche ionization in air surrounding the radioactive source when the laser beam is directed on the radioactive source from a selected distance;
a second laser source configured to generate a laser probe beam modulated by the avalanche ionization; and
a spectrometer configured to measure, based on a time evolution of electron density near the radioactive target of interest, a frequency modulation of the laser probe beam caused by the avalanche ionization.

19. The system of claim 18 , wherein a radioactive composition of the radioactive source is determined by:
measuring a frequency modulation of the laser probe beam,
determining, based on the frequency modulation, an electromagnetic signature of the radioactive source, and
identifying, based on the electromagnetic signature, the radioactive source as having a specific type of radioactive material.

20. The system of claim 19 , wherein the first laser source has a peak intensity of I peak =160 GW/cm 2 and a pulse duration of τ laser =1 sec.

Assignees

• Nusinovich Gregory
• Us Navy

Inventors

• Sprangle Phillip A
• Hafizi Bahman
• Zigler Arie
• Nusinovich Gregory
• Milchberg Howard

Classifications

• G01T7/00

  Details of radiation-measuring instruments · CPC title

• G01V8/005 Primary

  operating with millimetre waves, e.g. measuring the black losey radiation · CPC title

• G01T1/00 Primary

  Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation (G01T3/00, G01T5/00 take precedence) · CPC title