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:
May. 09, 2017

Filed:

Nov. 17, 2016
Applicant:

The United States of America As Represented BY the Secretary of the Air Force, Washington, DC (US);

Inventors:

Leanne J. Henry, Albuquerque, NM (US);

Thomas M. Shay, Saint George, UT (US);

Gerald T. Moore, Albuquerque, NM (US);

Jacob R. Grosek, Albuquerque, NM (US);

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
H01S 3/30 (2006.01); H01S 3/067 (2006.01); H01S 3/23 (2006.01); H01S 3/16 (2006.01); H01S 5/50 (2006.01); H01S 3/108 (2006.01);
U.S. Cl.
CPC ...
H01S 3/302 (2013.01); H01S 3/0675 (2013.01); H01S 3/06725 (2013.01); H01S 3/06754 (2013.01); H01S 3/108 (2013.01); H01S 3/1086 (2013.01); H01S 3/1655 (2013.01); H01S 3/2316 (2013.01); H01S 3/30 (2013.01); H01S 5/5027 (2013.01);
Abstract

A desired N-order Stokes output and zeroth-order Stokes pump input are seeded into a rare-earth doped amplifier where the power of the zeroth-order Stokes signal is amplified prior to both signals entering a Raman amplifier comprised of N−1 Raman resonators, each uniquely tuned to one of the N−1 Stokes orders, in various configurations to include one or more nested and/or in-series Raman resonators. The zeroth-order Stokes signal is converted to the N−1-order Stokes wavelength in steps and the power level of the N-order Stokes wavelength is amplified as the two signals propagate through the Raman resonators. Each Raman resonator includes a photosensitive Raman fiber located between a pair of Bragg gratings. The linewidths of the Stokes orders can be controlled by offsetting the reflectivity bandwidths of each pair of Bragg gratings respectively located in the Raman resonators.


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