Passive mode-locked laser system and method for generation of long pulses

Patent metadata

Field	Value
Publication number	US-10177525-B2
Application number	US-201615551709-A
Country	US
Kind code	B2
Filing date	Mar 15, 2016
Priority date	Mar 19, 2015
Publication date	Jan 8, 2019
Grant date	Jan 8, 2019

Abstract

A passive mode-locked laser method and system, the system comprising a nonlinear optical loop comprising a resonant nonlinear element, coupled to an amplification section by a beam splitter, the beam splitter splitting a light beam from the amplification section into light beams propagating in opposite directions around the nonlinear optical loop, the resonant nonlinear element acting as both a nonlinear element and a narrow bandwidth filter for the laser system, allowing mode-locking operation of the system on a single resonance of the resonant nonlinear element.

First claim

The invention claimed is:

1. A passive mode-locked laser system, comprising:
a nonlinear optical loop comprising a resonant nonlinear element;
an amplification section; and
an output coupler coupling optical pulses out of the laser system;
wherein said nonlinear optical loop and said amplification section are coupled together by a beam splitter, said beam splitter splitting a light beam from said amplification section into light beams propagating in opposite directions around said nonlinear optical loop; said resonant nonlinear element acting as both a nonlinear element and a narrow bandwidth filter for the laser system, allowing mode-locking operation of the system on a single resonance of the resonant nonlinear element.

2. The laser system of claim 1 , wherein said resonant nonlinear element is a third-order nonlinear material.

3. The laser system of claim 1 , wherein said resonant nonlinear element is one of: a nonlinear optical guided loop, a micro-toroid resonator, a micro-sphere resonator, a nonlinear Fabry-Perot cavity, a nonlinear Ikeda cavity, and a whispering gallery mode resonator.

4. The laser system of claim 1 , wherein said resonant nonlinear element is made in one of: silica-based glasses, silicon, silicon nitride and diamond.

5. The laser system of any one of claim 1 , wherein said beam splitter is a balanced beam splitter and said nonlinear optical loop operates as a nonlinear amplifying loop mirror.

6. The laser system of any one of claim 1 , wherein said beam splitter is a balanced beam splitter and said nonlinear optical loop comprises an optical gain element, a first one of said light beams propagating in opposite directions being first amplified by said optical gain element before entering said resonant nonlinear element, while a second one of said light beams propagating in opposite directions first passes said resonant nonlinear element and is then amplified by said optical gain element, said light beams propagating in opposite directions returning to said balanced beam splitter with a same amplitude and a nonlinear phase shift relative to one another, high intensity portions of said beams hitting said beam splitter being transmitting through said balanced beam splitter to said amplification section.

7. The laser system of claim 1 , wherein said beam splitter is a balanced beam splitter and said nonlinear optical loop comprises an optical gain element, a first one of said light beams propagating in opposite directions being first amplified by said optical gain element before entering said resonant nonlinear element, while a second one of said light beams propagating in opposite directions first passes said resonant nonlinear element and is then amplified by said optical gain element, said light beams propagating in opposite directions returning to said balanced beam splitter with a same amplitude and a nonlinear phase shift relative to one another, high intensity portions of said beams hitting said beam splitter being transmitting through said balanced beam splitter to said amplification section; and said amplification section is a unidirectional loop and comprises an optical gain element.

8. The laser system of claim 1 , wherein said amplification section comprises a first optical gain element, said nonlinear optical loop comprises a second optical gain element, a first one said light beams propagating in opposite directions being first amplified by said second optical gain element before entering said resonant nonlinear element, while a second one of said light beams propagating in opposite directions first passes said resonant nonlinear element and is then amplified by said second optical gain element, said light beams propagating in opposite directions returning to said balanced beam splitter with a same amplitude and a nonlinear phase shift relative to one another, high intensity portions of said light beams hitting said balanced beam splitter being transmitting through said balanced beam splitter to said amplification section.

9. The laser system of claim 1 , wherein said amplification section comprises a first optical gain element, said nonlinear optical loop comprises a second optical gain element, a first one said light beams propagating in opposite directions being first amplified by said second optical gain element before entering said resonant nonlinear element, while a second one of said light beams propagating in opposite directions first passes said resonant nonlinear element and is then amplified by said second optical gain element, said light beams propagating in opposite directions returning to said balanced beam splitter with a same amplitude and a nonlinear phase shift relative to one another, high intensity portions of said light beams hitting said balanced beam splitter being transmitting through said balanced beam splitter to said amplification section, and said first and second optical gain media are ones of: semiconductor optical amplifiers and Erbium doped fiber amplifiers.

10. The laser system of claim 1 , wherein said beam splitter is a balanced beam splitter, said amplification section comprises a first optical gain element and a first bandpass filter, said nonlinear optical loop comprises a second optical gain element and a second bandpass filter, a first one of said light beams propagating in opposite directions being first amplified by said second optical gain element before entering said resonant nonlinear element, while a second one of said light beams propagating in opposite directions first passes said resonant nonlinear element and is then amplified by said second optical gain element, said light beams propagating in opposite directions returning to said balanced beam splitter with a same amplitude and a nonlinear phase shift relative to one another, high intensity portions of said light beams propagating in opposite directions hitting said balanced beam splitter being transmitting through said balanced beam splitter to said amplification section, said first and second bandpass filters selecting a single resonance of said nonlinear resonant element and filtering noise of said first and second optical gain media respectively.

11. The laser system of claim 1 , wherein said output coupler is a beam splitter incorporated in said amplification section.

12. The laser system of claim 1 , wherein said beam splitter is an unbalanced beam splitter and said nonlinear optical loop operates as a nonlinear optical loop mirror.

13. The laser system of claim 1 , wherein said beam splitter is an unbalanced beam splitter and said nonlinear optical loop operates as a nonlinear optical loop mirror, and said amplification section comprises an optical gain element and a mirror.

14. The laser system of claim 1 , wherein said beam splitter is an unbalanced beam splitter and said nonlinear optical loop operates as a nonlinear optical loop mirror, and said output coupler is an unused port of said unbalanced beam splitter.

15. The laser system of claim 1 , wherein said beam splitter is an unbalanced beam splitter and said nonlinear optical loop operates as a nonlinear optical loop mirror, and said output coupler is a coupling element in said amplification section.

16. A source of mode-locked pulses in a range between 0.1 ns and 10 ns, comprising a nonlinear resonant element embedded in a nonlinear optical loop coupled to an amplification section by one of: i) a balanced beam splitter and ii) an unbalanced beam splitter; wherein the nonlinear optical loop operates as one of: i) a nonlinear amplifying loop mirror and ii) an unbalanced nonlinear optical loop mirror, respectively.

Assignees

• Inst Nat Rech Scient

Inventors

• Jestin Yoann
• Morandotti Roberto
• Kues Michael
• Wetzel Benjamin
• Reimer Christian
• Roztocki Piotr

Classifications

• H01S3/1112

  Passive mode locking · CPC title

• H01S3/0078

  Frequency filtering · CPC title

• H01S3/108

  using non-linear optical devices, e.g. exhibiting Brillouin or Raman scattering {(mode locking using a non-linear element H01S3/1112)} · CPC title

• G02B6/29338

  Loop resonators · CPC title

• H01S5/14

  External cavity lasers (H01S5/18 takes precedence; mode locking H01S5/065) · CPC title