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. 24, 2015

Filed:

Oct. 02, 2012
Applicant:

Commissariat À L'energie Atomique ET Aux Energies Alternatives, Paris, FR;

Inventors:

Dmitry Melyukov, Paris, FR;

Pierre-Yves Thro, Paris, FR;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G01B 11/08 (2006.01); G01J 1/42 (2006.01); G01B 17/00 (2006.01); G01N 25/02 (2006.01);
U.S. Cl.
CPC ...
G01B 11/08 (2013.01); G01B 17/00 (2013.01); G01J 1/4257 (2013.01); G01N 25/02 (2013.01);
Abstract

The invention relates to a method for measuring a ray rof a radiation beam (), characterized in that it comprises the steps according to which a source () of a radiation beam () excites (S) a standard member () via heat, in a periodic manner at a frequency (f), thereby obtaining a periodic thermal excitation of the standard member (); a sensor () measures (S) a periodic thermal response on the part of the standard member, in response to the periodic thermal excitation; a processor () determines (S) a phase shift (φ) between the periodic thermal excitation and the periodic thermal response; the source () exciting the standard member for a plurality of frequencies (f) and the processor () determining a phase shift for each frequency (f), and thereby determining a plurality of phase shifts (φ); the processor () determines (S) a minimum φ min of the phase shift (φ) thanks to the plurality of phase shifts determined in this manner, and determines (S) the ray rof the beam () via the following formula: r/g(φ) where Δ is the thickness of the standard member () and where g is a function dependent on the type of heat radiation beam ().


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