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:
Jun. 13, 2023

Filed:

Mar. 31, 2021
Applicant:

Ferdinand-braun-institut Ggmbh Leibniz-institut Für Höchstfrequenztechnik, Berlin, DE;

Inventors:

Anissa Zeghuzi, Berlin, DE;

Jan-Philipp Koester, Berlin, DE;

Hans Wenzel, Berlin, DE;

Heike Christopher, Berlin, DE;

Andrea Knigge, Königs Wusterhausen, DE;

Attorneys:
Primary Examiner:
Int. Cl.
CPC ...
H01S 5/065 (2006.01); H01S 5/042 (2006.01); H01S 5/22 (2006.01); H01S 5/40 (2006.01);
U.S. Cl.
CPC ...
H01S 5/0421 (2013.01); H01S 5/0653 (2013.01); H01S 5/222 (2013.01); H01S 5/4062 (2013.01); H01S 2301/18 (2013.01);
Abstract

The present disclosure relates to a diode laser having reduced beam divergence. Some implementations reduce a beam divergence in the far field by means of a deliberate modulation of the real refractive index of the diode laser. An area of the diode laser (e.g., the injection zone), may be structured with different materials having different refractive indices. In some implementations, the modulation of the refractive index makes it possible to excite a supermode, the field of which has the same phase (in-phase mode) under the contacts. Light, which propagates under the areas of a lower refractive index, obtains a phase shift of π after passing through the index-guiding trenches. Consequently, the in-phase mode is supported and the formation of the out-of-phase mode is prevented. Consequently, the laser field can, in this way, be stabilized even at high powers such that only a central beam lobe remains in the far field.


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