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:
Oct. 23, 2018

Filed:

Apr. 25, 2016
Applicant:

Honeywell International Inc., Morris Plains, NJ (US);

Inventor:

Robert Compton, Loretto, MN (US);

Assignee:

Honeywell International Inc., Morris Plains, NJ (US);

Attorney:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G01V 7/00 (2006.01); G01V 7/02 (2006.01); G01B 9/02 (2006.01); G01P 15/08 (2006.01); G01P 15/093 (2006.01); G01N 21/64 (2006.01);
U.S. Cl.
CPC ...
G01V 7/00 (2013.01); G01B 9/02003 (2013.01); G01B 9/02045 (2013.01); G01P 15/0802 (2013.01); G01P 15/093 (2013.01); G01V 7/02 (2013.01); G01B 2290/25 (2013.01); G01B 2290/70 (2013.01); G01N 21/64 (2013.01);
Abstract

An atomic interferometric accelerometer comprises a laser that emits a pulsed beam at a first frequency, an electro-optic modulator that receives the beam, and a vacuum cell in communication with the electro-optic modulator. The electro-optic modulator outputs a first optical signal corresponding to the beam at the first frequency and a second optical signal having a second frequency different from the first frequency. The vacuum cell has a chamber for laser cooled atoms. The vacuum cell receives the optical signals such that they propagate in a direction that passes through the atoms. A piezo mirror retro-reflects the optical signals back through the vacuum cell in a counter-propagating direction. The piezo mirror is driven with substantially constant velocity during a beam pulse, thereby imparting a Doppler shift to the retro-reflected optical signals to create two non-symmetric counter-propagating lightwave pairs. One of the lightwave pairs supports interferometry while the other is non-resonant.


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