Short pulsed IR fiber laser at wavelength > 2 μm

Patent metadata

Field	Value
Publication number	US-9570873-B2
Application number	US-201313742566-A
Country	US
Kind code	B2
Filing date	Jan 16, 2013
Priority date	Jan 19, 2012
Publication date	Feb 14, 2017
Grant date	Feb 14, 2017

Abstract

A method of generating ultrashort pulses with wavelengths greater than 2 μm comprising a short pulse diode laser or fiber laser operating at a wavelength of 1 μm or greater with a pulse width of 10 ps or greater, one or more amplification stages to increase the peak power of the pulsed source, a nonlinear fiber stage whereby the dispersion of the nonlinear fiber is anomalous at the pulsed source wavelength such that the fiber breaks up the pulse into a series of sub-ps pulse train through modulation instability which may be seeded by spontaneous noise which are then wavelength shifted in one or more stages by soliton self frequency shift in anomalous dispersion fiber or Raman in normal dispersion fiber and amplified in one or more stages to generate a high peak power ultrashort pulse (<1 ps) source at a wavelength of 2.4 μm or greater.

First claim

What is claimed as new and desired to be protected by Letters Patent of the United States is:

1. A method for generating ultrashort infrared pulses, comprising:
using a laser to generate one or more pulses;
amplifying the pulse in one or more amplification stages, wherein amplifier materials are selected from one stage to the next with overlapping absorption bands thereby removing the need for optical isolators;
pumping the amplified pulse into one or more nonlinear fibers whereby the fiber breaks up the pulse into a pulse train that is 1 ps or less;
wavelength shifting the pulse train one or more times; and
amplifying the wavelength shifted pulse train to a wavelength of 2.4 μm or greater.

2. The method of claim 1 , wherein the laser generates a pulse with a wavelength of 1 μm or greater.

3. The method of claim 1 , wherein the laser generates a pulse with a pulse width of 10 ps or greater.

4. The method of claim 1 , wherein the wavelength shifting is done by soliton self frequency shift in anomalous dispersion fiber or Raman in normal dispersion fiber.

5. The method of claim 1 , wherein the laser is a diode laser or a fiber laser.

6. The method of claim 1 , wherein amplification is achieved with fiber amplifiers, semiconductor optical amplifiers, bulk nonlinear crystal optical parametric amplifiers, or any combination thereof.

7. The method of claim 1 , wherein the laser generates a pulse with a pulse width of less than 1 ps and wherein the amplified pulse does not have to be pumped into one or more nonlinear fibers to break up the pulse into a pulse train.

8. The method of claim 1 , wherein amplifying the pulse, pumping the amplified pulse, and wavelength shifting the pulse train are combined into a single step.

9. The method of claim 1 , wherein the wavelength shifted pulse train has a high peak power of greater than 10 kW.

10. A system for generating ultrashort infrared pulses, comprising:
a laser to generate one or more pulses;
one or more amplifiers to amplify the pulse, wherein amplifier materials are selected from one stage to the next with overlapping absorption bands thereby removing the need for optical isolators; and
one or more nonlinear fibers into which the amplified pulse is pumped whereby the fiber breaks up the pulse into a pulse train that is 1 ps or less, wherein the pulse train is wavelength shifted one or more times, and wherein the wavelength shifted pulse train is amplified to a wavelength of 2.4 μm or greater.

11. The system of claim 10 , wherein the laser generates a pulse with a wavelength of 1 μm or greater.

12. The system of claim 10 , wherein the laser generates a pulse with a pulse width of 10 ps or greater.

13. The system of claim 10 , wherein the wavelength shifting is done by soliton self frequency shift in anomalous dispersion fiber or Raman in normal dispersion fiber.

14. The system of claim 10 , wherein the laser is a diode laser or a fiber laser.

15. The system of claim 10 , the amplifier is a fiber amplifier, semiconductor optical amplifier, bulk nonlinear crystal optical parametric amplifier, or any combination thereof.

16. The system of claim 10 , wherein the laser generates a pulse with a pulse width of less than 1 ps and wherein the amplified pulse does not have to be pumped into one or more nonlinear fibers to break up the pulse into a pulse train.

17. The system of claim 10 , wherein amplifying the pulse, pumping the amplified pulse, and wavelength shifting the pulse train are combined.

18. The system of claim 10 , wherein the wavelength shifted pulse train has a high peak power of greater than 10 kW.

Assignees

• Shaw Leslie Brandon
• Gattass Rafael R
• Sanghera Jasbinder S
• Aggarwal Ishwar D
• Us Navy

Inventors

• Shaw Leslie Brandon
• Gattass Rafael R
• Sanghera Jasbinder S
• Aggarwal Ishwar D

Classifications

• H01S3/0057 Primary

  Temporal shaping, e.g. pulse compression, frequency chirping (soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108) · CPC title

• 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

• H01S3/06758 Primary

  Tandem amplifiers · CPC title

• H01S3/0672

  Non-uniform radial doping · CPC title

• H01S3/1616

  thulium · CPC title