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. 21, 2019

Filed:

Feb. 07, 2018
Applicant:

Max-planck-gesellschaft Zur Foerderung Der Wissenschaften E. V., Munich, DE;

Inventors:

Thomas Udem, Munich, DE;

Akira Ozawa, Garching bei Munich, DE;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G01J 3/02 (2006.01); G01J 3/10 (2006.01); G01J 3/28 (2006.01); G01J 9/04 (2006.01); H01S 3/00 (2006.01); H01S 3/11 (2006.01); G01J 3/433 (2006.01); G01N 21/39 (2006.01); H01S 3/067 (2006.01);
U.S. Cl.
CPC ...
H01S 3/1121 (2013.01); G01J 3/0218 (2013.01); G01J 3/10 (2013.01); G01J 3/4338 (2013.01); G01J 9/04 (2013.01); G01N 21/39 (2013.01); H01S 3/0057 (2013.01); H01S 3/0675 (2013.01); H01S 3/06791 (2013.01); H01S 3/1109 (2013.01); H01S 3/1112 (2013.01); G01J 2003/282 (2013.01); G01J 2003/4332 (2013.01); G01N 2021/391 (2013.01); G01N 2021/399 (2013.01); G01N 2201/0697 (2013.01);
Abstract

A method of generating laser pulses () includes: creating a circulating light field in resonator device () having resonator length L and an intra-cavity dispersion and configured for supporting light field resonator modes, and generating a pulse train of laser pulses () by a mode-locking mechanism. Laser pulses () are generated with a repetition frequency and provide a frequency comb with carrier frequency ωand comb modes in frequency space. The intra-cavity dispersion is selected such that round trip phases ϕ have a dependency on frequency ω according to wherein m is an integer providing effective repetition rate (mω) in combination with mode spacing ωat optical carrier frequency (ω), and the mode-locking mechanism provides a coupling of the resonator modes whereby frequency difference (Δn=ω−ω) between neighboring mode frequencies (ω, ω) is a linear function of mode frequency number n. Furthermore, a spectroscopy method for investigating a sample, a laser pulse source apparatus and a spectroscopy apparatus are described.


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