Active stabilization of mode instabilities in optical waveguides

Patent metadata

Field	Value
Publication number	US-10490969-B2
Application number	US-201715649754-A
Country	US
Kind code	B2
Filing date	Jul 14, 2017
Priority date	Jul 15, 2016
Publication date	Nov 26, 2019
Grant date	Nov 26, 2019

Abstract

A method of propagating a laser signal through an optical waveguide and a waveguide laser system provide a novel way of stabilizing the beam emitted by a fiber laser system above the mode instability threshold wherein the beat length of two or more interfering transverse modes of the laser signal in the optical waveguide is modulated in time.

First claim

What is claimed is:

1. A method of propagating a laser signal through an optical waveguide, wherein a beat length of two or more transverse modes of the laser signal in the optical waveguide is modulated and wherein an amplitude, a frequency, and/or a temporal shape of the modulation of the beat length of the transverse modes is controlled by a feedback loop which monitors the laser signal at an output of the optical waveguide.

2. The method of claim 1 , wherein the beat length is modulated with a frequency below 100 kHz.

3. The method of claim 1 , wherein the beat length of the transverse modes is modulated with a frequency below 10 kHz.

4. The method of claim 1 , wherein the optical waveguide is optically active and is optically pumped to amplify the laser signal while propagating through the optical waveguide.

5. The method of claim 4 , wherein the modulation of the beat length of the transverse modes is achieved by modulating a pump power.

6. The method of claim 5 , wherein at least two pump sources are used, wherein a pump radiation of one of the pump sources propagates in a co-propagating direction and the pump radiation of another one of the pump sources propagates in a counter-propagating direction with respect to the laser signal through the optical waveguide.

7. The method of claim 6 , wherein the modulation of the pump power of the pump sources is synchronized to achieve a constant power of the laser signal at an output of the optical waveguide.

8. The method of claim 4 , wherein the modulation of the beat length of the transverse modes is achieved by modulating the power of the laser signal coupled into the optical waveguide.

9. The method of claim 4 , wherein a modulated auxiliary signal is coupled into the optical waveguide in addition to the laser signal, wherein the wavelength of the auxiliary signal falls within the amplification bandwidth of the optical waveguide.

10. The method of claim 4 , wherein the optical waveguide comprises an absorbing material which is illuminated by an external modulated radiation source at an absorption wavelength of the absorbing material, wherein the absorption wavelength is outside of the pump absorption bands and amplification bands of the optical waveguide.

11. The method of claim 10 , wherein the absorbing material is the host material of the optical waveguide.

12. The method of claim 1 , wherein two or more electrodes are incorporated into the optical waveguide, wherein a modulated voltage is applied to the electrodes to dynamically modify the refractive index profile of the optical waveguide via electrostriction.

13. The method of claim 1 , wherein the optical waveguide is doped with rare-earth ions.

Assignees

• Fraunhofer Ges Forschung
• Univ Jena Friedrich Schiller

Inventors

• Stihler Christoph
• Jáuregui Misas César
• Limpert Jens
• Otto Hans-Juergen
• Tuennermann Andreas
• Stutzki Fabian

Classifications

• G02F1/365

  in an optical waveguide structure (G02F1/377, {G02F1/395} take precedence) · CPC title

• H01S3/094076

  Pulsed or modulated pumping (H01S3/1024 takes precedence) · CPC title

• H01S3/13013

  by controlling the optical pumping · CPC title

• H01S3/10015

  by monitoring or controlling, e.g. attenuating, the input signal · CPC title

• H01S3/10013

  by controlling the temperature of the active medium · CPC title