High-Repetition-Rate Guided-Mode Femtosecond Laser

• US 20090310631A1
• Filed: 06/01/2009
• Published: 12/17/2009
• Est. Priority Date: 06/11/2008
• Status: Active Grant

• Current Assignee: Massachusetts Institute of Technology
• Original Assignee: Massachusetts Institute of Technology
• Inventors: Pudo, Dominik, Byun, Hyunil, Chen, Jian, Kaertner, Franz X., Ippen, Erich P.
• Granted Patent: US 8,194,709 B2
• Time in Patent Office: Days
• US Class Current: 372/21
• CPC Class Codes: H01S 2301/085 solitons
• CPC Class Codes: H01S 3/0632 Thin film lasers in which light propagates in the plane of the thin film
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/06725 Fibre characterized by a specific dispersion, e.g. for pulse shaping in soliton lasers or for dispersion compensating [DCF]
• CPC Class Codes: H01S 3/06741 Photonic crystal fibre, i.e. the fibre having a photonic bandgap
• CPC Class Codes: H01S 3/06791 Fibre ring lasers fibre laser gyrometers G01C19/72
• CPC Class Codes: H01S 3/1115 using intracavity saturable absorbers
• CPC Class Codes: H01S 3/2308 Amplifier arrangements, e.g. MOPA

Abstract

Femtosecond pulse trains in waveguide lasers with high fundamental repetition rates are achieved by exploiting the nonlinearity in the waveguide. Components of the apparatus include an optical resonator, a saturable absorber for starting and stabilizing mode-locking, and a gain element. Part of the laser cavity or the entire laser cavity is made of waveguide or fiber (collectively called “waveguide” herein). The net dispersion of the laser cavity can be anomalous. This anomalous dispersion in combination with the positive self-phase modulation nonlinearity in the waveguide creates soliton formation to shorten the pulse duration in the invented lasers. Conversely, a normal dispersive waveguide with negative self-phase modulation nonlinearity can also be used.

Claims

1. A method for generating a high-repetition-rate guided-mode femtosecond laser comprising:

providing a laser comprising the following cavity components;

a saturable absorption device, a reflector, and a waveguide extending between the saturable absorption device and the reflector;

providing an optical pulse that traverses the waveguide between the saturable absorption device and the reflector; and

producing a soliton from the optical pulse, the cavity components increasing the intensity of the pulse and providing a balance of dispersion and nonlinearity to provide the soliton with a pulsewidth of no more than 500 femtoseconds and a repetition rate of at least 500 MHz.

2. The method of claim 1, wherein the optical pulse is provided by injecting optical pump light through the reflector into the waveguide.

3. The method of claim 1, wherein the optical pulse is extracted from the cavity through the reflector.

4. The method of claim 1, wherein the length of the waveguide is no more than 6 cm.

5. The method of claim 1, wherein the pulse does not pass through any stretches of free space in the laser.

6. The method of claim 1, wherein the pulse does not pass through any lenses in the laser.

7. The method of claim 1, wherein the saturable absorption device has a recovery time of at most 10 ps.

8. The method of claim 1, wherein the waveguide comprises an active waveguide joined with a passive waveguide, wherein the passive waveguide provides dispersion or nonlinearity to compensate for or temper the dispersion or nonlinearity in the active waveguide.

9. The method of claim 1, wherein the reflector includes a coating that provides dispersion to compensate for or temper the dispersion in the waveguide.

10. The method of claim 1, wherein the pulse has a repetition rate of at least 1 GHz.

11. The method of claim 1, further comprising tuning the nonlinearity of the waveguide by adjusting the waveguide temperature or by adjusting the pump power.

12. The method of claim 1, wherein the cavity components provide negative dispersion and positive nonlinearity.

13. The method of claim 1, wherein the cavity components provide positive dispersion and negative nonlinearity.

14. A high-repetition-rate guided-mode femtosecond laser comprising:

a laser cavity;

a saturable absorption device in the laser cavity;

a partial reflector in the laser cavity; and

a waveguide extending between the saturable absorption device and the partial reflector in the cavity.

15. The high-repetition-rate guided-mode femtosecond laser of claim 14, wherein the waveguide has two opposite ends and is coupled at one end with the saturable absorption device and at the other end with the partial reflector.

16. The laser of claim 14, wherein the laser is a solid-state erbium laser.

17. The laser of claim 14, wherein the waveguide is a planar waveguide and not a fiber.

18. The laser of claim 14, wherein the saturable absorption device is a semiconductor saturable absorber.

19. The laser of claim 14, wherein the saturable absorption device comprises a second reflector and a saturable absorber, wherein the second reflector bounds the waveguide and the saturable absorber is positioned alongside the waveguide.

20. The laser of claim 14, wherein the saturable absorption device is structured to produce intensity-dependent loss in an optical pulse via the Kerr Effect.

21. The laser of claim 20, wherein the saturable absorption device comprises:

a directional coupler to split the input power;

two passive waveguide sections with different nonlinearities provided by different material selection or different mode area;

a directional coupler to combine the power from the two passive waveguide sections; and

an apparatus to induce an optical phase change over one of the said two passive waveguide sections.

22. The laser of claim 21, wherein the apparatus for inducing the optical phase change is a heating pad.