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:
Apr. 03, 1990

Filed:

Oct. 27, 1988
Applicant:
Inventors:

Krassimir Stankov, Goettingen, DE;

Fritz P Schafer, Goettingen, DE;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
H01S / ;
U.S. Cl.
CPC ...
372 18 ; 372 21 ; 372 99 ; 372108 ;
Abstract

Mode-locked laser comprising an active medium for the emission of a fundatal frequency radiation w1, with a resonator which is defined by a first mirror and a second mirror and in which the active medium is disposed, and a nonlinear optical means which is arranged between the active medium and the second mirror and which in combination with the second mirror effects a preferred reflection of radiation of higher intensity compared with radiation of lower intensity and it converts a fundamental-frequency radiation reversibly into radiation of a first frequency and radiation of a second frequency in such a manner that with increasing intensity the fraction of the radiation of the second frequency increases, and that the second mirror reflects at the second frequency to a greater extent than at the first frequency. A further development of said laser comprises a means for coupling laser radiation of a further frequency w2 into the nonlinear means and a reflector arrangement which is arranged in the path of radiation emerging from the nonlinear means and for the fundamental-frequency radiation w1 and the radiation of the other frequency has a lower reflectivity than for radiation (w1+w2; w1-w2) which arises by interaction of the two laser radiations in the nonlinear means. In this manner a simple synchronization of the mode-locked laser with the coupled-in laser radiation is possible. The coupled-in laser can originate from a second laser medium which is arranged in a second resonator which has a part in common with the first resonator.


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