Multiple wavelength Raman laser

Patent metadata

Field	Value
Publication number	US-9379516-B2
Application number	US-201514685368-A
Country	US
Kind code	B2
Filing date	Apr 13, 2015
Priority date	Apr 21, 2010
Publication date	Jun 28, 2016
Grant date	Jun 28, 2016

Abstract

A pulsed laser system may include a Raman fiber that is configured to act as multiple wavelength Raman laser. The fiber is configured to receive a pulsed input beam from an input source and convert the input beam to an output beam having narrow band outputs at first and second frequencies v 1 and v 2 .

First claim

What is claimed is:

1. A laser system, comprising:
an optical fiber configured to receive a pulsed input beam from an input source and convert the input beam to an output beam having outputs at two or more frequencies including a first frequency v 1 and a second frequency v 2 by Raman scattering;
a nonlinear material, wherein an output of the optical fiber is focused into the nonlinear material; and
a pulsed laser input source optically coupled to the optical fiber, wherein the pulsed input source is configured to provide the pulsed input beam, wherein the pulsed input beam is characterized by one or more pulses configured such that a figure of merit (FOM) for the one or more pulses is greater than about 60%, wherein the FOM is given by a percentage conversion of the input beam to the first frequency when the power at the second frequency is about 2% of an input power of the input beam.

2. The system of claim 1 , wherein the nonlinear material is a nonlinear crystal.

3. The system of claim 2 , wherein the nonlinear crystal is a periodically poled material.

4. The system of claim 3 wherein the periodically poled material is a periodically poled lithium niobate (PPLN) crystal.

5. The system of claim 4 wherein the PPLN crystal is doped with magnesium oxide (MgO).

6. The system of claim 3 , wherein the periodically poled material includes two or more poling regions arranged side-by-side, wherein each poling region is configured for a different non-linear frequency conversion.

7. The system of claim 1 , wherein the nonlinear material is a periodically poled material having two or more poling regions that include a first poling region configured for frequency doubling of the first frequency v 1 , a second poling region configured for frequency doubling of the second frequency v 2 , and a third poling region configured for frequency summing of the first and second frequencies v 1 and v 2 .

8. The system of claim 1 , further comprising a translation stage, wherein the nonlinear material is a periodically poled material and the periodically poled material is mounted to the translation stage, wherein the translation stage is configured to translate the periodically poled material with respect to the output beam to align the output beam with a desired poling region.

9. The system of claim 8 wherein a distance between the first and second gratings is configured such that a round trip time between the gratings is an integer multiple of a time between pulses of the input beam.

10. The system of claim 1 , further comprising a first grating proximate an input end of the optical fiber and a second grating region proximate an output end of the fiber, wherein the gratings are configured to reflect the first and second frequency outputs but to transmit the input beam.

11. The system of claim 10 wherein the gratings are configured to reflect light over a bandwidth of about 1 nm or less at the first frequency v 1 and the second frequency v 2 .

12. The system of claim 10 wherein the first grating has a reflectivity greater than about 95% and the second grating has a reflectivity between about 1% and about 5%.

13. The system of claim 10 wherein the first and second gratings are configured to reflect radiation corresponding to two or more Raman wavelengths generated in the optical fiber.

14. The system of claim 10 further comprising a passive optical fiber optically having an input end and an output end, wherein the output end is optically coupled to the input of the optical fiber, wherein the passive optical fiber is configured to convert at least a portion of a pump radiation by the Raman effect to generate the input beam.

Assignees

• Ipg Ipg Photonics Corp
• Ipg Photonics Corp

Inventors

• Keaton Gregory L
• Leonardo Manuel J
• Byer Mark W
• Monro Kiyomi

Classifications

• H01S3/0092

  Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity (nonlinear frequency conversion per se G02F1/35) · CPC title

• G02F1/3532

  Arrangements of plural nonlinear devices for generating multi-colour light beams, e.g. arrangements of SHG, SFG, OPO devices for generating RGB light beams · CPC title

• H01S3/08086

  Multiple-wavelength emission · CPC title

• H01S3/302 Primary

  in an optical fibre · CPC title

• H01S3/06754

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