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:
Feb. 27, 2024

Filed:

May. 04, 2021
Applicants:

King Abdullah University of Science and Technology, Thuwal, SA;

Politecnico Di Milano, Milan, IT;

Inventors:

Mohammad Khaled Shakfa, Thuwal, SA;

Marco Lamperti, Lecco, IT;

Marco Marangoni, Lecco, IT;

Aamir Farooq, Thuwal, SA;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G02F 1/35 (2006.01); G02F 1/355 (2006.01); H01S 5/00 (2006.01); H01S 3/00 (2006.01); H01S 3/223 (2006.01); H01S 5/14 (2006.01); G01J 3/10 (2006.01); H01S 5/34 (2006.01);
U.S. Cl.
CPC ...
G02F 1/3505 (2021.01); G01J 3/108 (2013.01); G02F 1/3503 (2021.01); G02F 1/3551 (2013.01); G02F 1/3556 (2013.01); G02F 1/3558 (2013.01); H01S 3/0092 (2013.01); H01S 3/2232 (2013.01); H01S 5/0092 (2013.01); H01S 5/14 (2013.01); H01S 5/3402 (2013.01); G02F 2202/101 (2013.01); G02F 2203/11 (2013.01);
Abstract

A laser source includes a first laser device configured to generate a first laser beam having a first wavelength, a second laser device configured to generate a second laser beam having a second wavelength, which is different from the first wavelength, and a non-linear crystal configured to receive simultaneously the first and second laser beams and to generate a third laser beam that has a third wavelength, which is larger than each of the first and second wavelengths. The non-linear crystal has a length and a width, and a variable poling period is distributed across the width so that the third wavelength varies within a given wavelength range based on an incident position of the first and second laser beams along the width of the non-linear crystal.


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