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:
Mar. 29, 2022

Filed:

Feb. 07, 2020
Applicant:

Institut National DE LA Recherche Scientifique, Quebec, CA;

Inventors:

Riccardo Piccoli, Montreal, CA;

Bruno E. Schmidt, Montreal, CA;

Luca Razzari, Mont-Royal, CA;

Younggyun Jeong, Montreal, CA;

Roberto Morandotti, Montreal, CA;

Attorneys:
Primary Examiner:
Int. Cl.
CPC ...
H01S 3/00 (2006.01); G02F 1/35 (2006.01); H01S 3/03 (2006.01); H01S 3/30 (2006.01); G02B 27/14 (2006.01); G02F 1/355 (2006.01); G02F 1/365 (2006.01);
U.S. Cl.
CPC ...
H01S 3/0092 (2013.01); G02F 1/3503 (2021.01); G02F 1/353 (2013.01); G02F 1/3507 (2021.01); H01S 3/0057 (2013.01); H01S 3/0315 (2013.01); G02B 27/14 (2013.01); G02F 1/3551 (2013.01); G02F 1/365 (2013.01); H01S 3/305 (2013.01);
Abstract

A system and a method for generating tunable ultrafast optical pulses, the method comprising spectral broadening of a laser input beam by propagating the laser input beam in a nonlinear medium of a third-order nonlinear susceptibility χ, yielding an output laser spectrum; and one of: i) selecting at least one portion of the output laser spectrum, yielding an output pulse different than the input pulse and centered at a different frequency; ii) temporal compensation and spatial spreading of spectral components of the output laser spectrum; selecting two pulses at two different frequencies; and nonlinearly mixing the two pulses together in a first second-order nonlinear susceptibility χnonlinear crystal into a third pulse centered at a frequency which is a difference between the frequencies of the first two pulses; and iii) dividing output laser spectrum into a pump beam and a probe beam, directing a pump pulse to a third second-order nonlinear crystal for THz radiation generation; and directing a probe pulse to a third second-order nonlinear crystal for THz radiation reconstruction.


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