The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Nov. 18, 2014

Filed:

Aug. 04, 2010
Applicants:

Robert L. Rosson, Atlanta, GA (US);

Bernd Kahn, Atlanta, GA (US);

Brent Wagner, Marietta, GA (US);

David Roberts, Smyrna, GA (US);

Inventors:

Robert L. Rosson, Atlanta, GA (US);

Bernd Kahn, Atlanta, GA (US);

Brent Wagner, Marietta, GA (US);

David Roberts, Smyrna, GA (US);

Assignee:
Attorneys:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G01T 1/205 (2006.01); G01T 7/00 (2006.01); G01N 21/64 (2006.01); G01S 17/88 (2006.01); G01N 21/17 (2006.01); G01N 21/47 (2006.01); G01S 17/95 (2006.01);
U.S. Cl.
CPC ...
G01T 7/00 (2013.01); G01N 21/6402 (2013.01); G01S 17/88 (2013.01); G01N 2021/1793 (2013.01); G01N 2021/4709 (2013.01); G01N 2021/6419 (2013.01); G01S 17/95 (2013.01);
Abstract

Various embodiments of the present invention provide a method of detecting inaccessible radiation sources by measuring corresponding ions and excited molecules created by radiation, using LIDAR technology. The LIDAR system of the present invention employs a pulsed laser transmitter, a telescope receiver, and associated control and acquisition systems. Light propagates out from the laser transmitted and is directed into the volume surrounding the radioactive source, or the 'ion cloud.' The ion cloud absorbs the transmitted light, which induces the non-fluorescing ions to fluoresce. Light from the ion cloud is then backscattered and the telescope receiver subsequently collects the photons from the backscattered light. The intensity of the fluorescence (determined by the photon count) is measured, which provides an indication of the number density of the ionized atoms. Algorithms can then be used to relate the measured ionization rates to the source activity.


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