Optical waveguide as amplifier fibre for high-performance operation

Patent metadata

Field	Value
Publication number	US-10340655-B2
Application number	US-201515549416-A
Country	US
Kind code	B2
Filing date	Feb 12, 2015
Priority date	Feb 9, 2015
Publication date	Jul 2, 2019
Grant date	Jul 2, 2019

Abstract

The invention relates to an optical waveguide ( 3 ) as a laser medium or as a gain medium for high-power operation, wherein the optical waveguide ( 3 ) is an optical fiber, the light-guiding core of which, at least in sections, is doped with rare earth ions. It is an object of the invention to provide an optical waveguide as a laser or a gain medium, and a laser/amplifier combination realized therewith, in which the output signal of the laser or gain medium is better stabilized. The invention achieves this object by virtue of the maximum small signal gain of the optical waveguide ( 1 ) being up to 60 dB, preferably up to 50 dB, more preferably up to 40 dB, even more preferably up to 30 dB, on account of the concentration of the rare earth ions and/or the distribution thereof in the light-guiding core. Moreover, the invention relates to the use of such an optical waveguide as an amplifier fiber ( 3 ) in a laser/amplifier combination.

First claim

The invention claimed is:

1. A laser/amplifier device comprising a laser, an amplifier fiber and a pump light source, wherein the pump light source optically pumps the amplifier fiber and wherein the amplifier fiber amplifies the radiation of the laser-propagating therein, wherein the core of the amplifier fiber guiding the laser radiation, at least in sections, is doped with rare earth ions, wherein the maximum small signal gain of the amplifier fiber is up to 60 dB on account of at least one of the concentration of the rare earth ions and the distribution thereof in the light-guiding core, and wherein the mean power of the laser radiation at the output of the amplifier fiber is at least 100 W.

2. The device of claim 1 , wherein the wavelength of the laser radiation lies away from the wavelength, at which the wavelength-dependent gain of the amplifier fiber is at maximum.

3. The device of claim 1 , wherein the wavelength of the light of the pump light source lies away from the wavelength, at which the absorption of the amplifier fiber is at maximum.

4. The device of claim 1 , wherein the mean power of the laser radiation at the output of the amplifier fiber is at least 500 W.

5. The device of claim 1 , wherein the mean power of the laser radiation at the output of the amplifier fiber is at least 1 kW.

6. The device of claim 1 , wherein the mean power of the laser radiation at the output of the amplifier fiber is at least 10 kW.

7. The device of claim 1 , wherein the wavelength of the laser radiation lies below the wavelength, at which the wavelength-dependent gain of the amplifier fiber is at maximum.

8. The device of claim 1 , wherein the maximum small signal gain of the amplifier fiber is up to 50 dB.

9. The device of claim 1 , wherein the maximum small signal gain of the amplifier fiber is up to 40 dB.

10. The device of claim 1 , wherein the maximum small signal gain of the amplifier fiber is up to 30 dB.

Assignees

• Fraunhofer Ges Forschung
• Univ Schiller Jena

Inventors

• Otto Hans Jurgen
• Jauregui Misas Cesar
• Limpert Jens
• Tunnermann Andreas

Classifications

• H01S3/06754

  Fibre amplifiers (H01S3/06708 takes precedence) · CPC title

• H01S3/06716

  Fibre compositions (per se C03C13/04)or doping with active elements (lasing materials in general H01S3/14) · CPC title

• H01S3/08072

  Thermal lensing or thermally induced birefringence; Compensation thereof · CPC title

• H01S3/1603 Primary

  rare earth · CPC title

• H01S3/091

  using optical pumping · CPC title