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:
Jun. 13, 2017

Filed:

Dec. 23, 2014
Applicant:

Trutag Technologies, Inc., Kapolei, HI (US);

Inventors:

Timothy Learmonth, Berkeley, CA (US);

Hod Finkelstein, El Cerrito, CA (US);

Assignee:

TruTag Technologies, Inc., Kapolei, HI (US);

Attorney:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G01J 3/45 (2006.01); G01J 3/26 (2006.01); G01J 3/02 (2006.01); G01N 21/25 (2006.01); G01J 3/10 (2006.01);
U.S. Cl.
CPC ...
G01J 3/26 (2013.01); G01J 3/0237 (2013.01); G01J 3/10 (2013.01); G01N 21/255 (2013.01); G01J 2003/102 (2013.01); G01N 2201/061 (2013.01);
Abstract

A system for wide-range spectral measurement includes one or more broadband sources, an adjustable Fabry-Perot etalon, and a detector. The one or more broadband sources is to illuminate a sample, wherein the one or more broadband sources have a short broadband source coherence length. The adjustable Fabry-Perot etalon is to optically process the reflected light to extract spectral information with fine spectral resolution. The detector is to detect reflected light from the sample, wherein the reflected light is comprised of multiple narrow-band subsets of the illumination light having long coherence lengths and is optically processed using a plurality of settings for the adjustable Fabry-Perot etalon, and wherein the plurality of settings includes a separation of the Fabry-Perot etalon plates that is greater than the broadband source coherence length but that is less than the long coherence lengths.


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