Technique for the generation of optical pulses in modelocked lasers by dispersive control of the oscillation pulse width

• US 5,450,427 A
• Filed: 10/21/1994
• Issued: 09/12/1995
• Est. Priority Date: 10/21/1994
• Status: Expired due to Term

• Current Assignee: IMRA America Incorporated (Aisin Corp.)
• Original Assignee: IMRA America Incorporated (Aisin Corp.)
• Inventors: Harter, Donald J., Fermann, Martin E.
• Primary Examiner(s): SCOTT JR, LEON
• Application Number:
  US08/326,928
• Time in Patent Office: 326 Days
• Field of Search: 372/18, 372/6, 372/102, 372/21, 372/27, 372/34, 372/64, 372/20, 372/700, 372/11-13
• US Class Current: 372/10
• CPC Class Codes: H01S 2301/085 solitons
• CPC Class Codes: H01S 3/0675 Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
• CPC Class Codes: H01S 3/06791 Fibre ring lasers fibre laser gyrometers G01C19/72
• CPC Class Codes: H01S 3/1055 one of the reflectors being constituted by a diffraction grating
• CPC Class Codes: H01S 3/1112 Passive mode locking
• CPC Class Codes: H01S 3/1118 Semiconductor saturable absorbers, e.g. semiconductor saturable absorber mirrors [SESAMs]; Solid-state saturable absorbers, e.g. carbon nanotube [CNT] based
• CPC Class Codes: H01S 3/1608 erbium

Abstract

The invention relates to modelocked lasers including highly dispersive optical elements. The dispersive optical elements increase the oscillation pulse width inside the laser oscillators, which reduces the nonlinearity of the laser cavity for a given oscillating pulse energy. Compared to conventionally designed modelocked lasers, an increase in output pulse energy by one to three orders is achieved. As way of example, the technique is applied to an erbium fiber laser, where a chirped fiber Bragg grating is employed as the dispersive element. By using a Kerr-modelocking technique, a high nonlinearity may be sustained inside the fiber laser cavity, which leads to the generation of pulses with psec widths and energies up to 2 nJ. The large bandwidth of the chirped fiber Bragg grating allows a wavelength tuning range in excess of 10 nm, which is achieved by polarization control and a control of the gain spectrum of the laser.

Claims

1. A modelocked laser comprising:

means for generating laser energy;

a gain medium for amplifying said laser energy within a laser cavity;

means for reflecting said energy along an axis which passes through the gain medium;

a modelocking mechanism for inducing modelocking of said laser, and sustaining a high non-linearity within the laser cavity;

means for outputting laser energy generated within said cavity; and

a dispersive delay line comprised of at least one chirped grating, for controlling a pulse width of said output laser energy.

2. A modelocked laser according to claim 1, wherein a plurality of chirped gratings of same or different dispersions are used as dispersive delay line elements.

3. A modelocked laser according to claim 2, wherein at least one of said plurality of chirped gratings further serves as said energy reflecting means.

4. A modelocked laser according to claim 1, further comprising an optical filter in said cavity for wavelength tuning.

5. A modelocked laser according to claim 1, further comprising wavelength tuning means including means for controlling intra-cavity loss and polarization state.

6. A modelocked laser according to claim 1, further comprising wavelength tuning means including means for inducing a change of reflectivity of said grating by changing an operating temperature of said grating or stretching of the grating.

7. A modelocked laser according to claim 1, further comprising wavelength tuning means including means for inducing a change of reflectivity of said grating by stretching of said grating.

8. A modelocked laser according to claim 1, wherein said chirped grating comprises a chirped fiber or waveguide grating.

9. A modelocked laser according to claim 1, wherein said gain medium comprises one of an optical fiber and optical waveguide, doped with a gain material.

10. A modelocked laser according to claim 9, further comprising a Faraday mirror for elimination of linear phase drifts between polarization eigenmodes of the fiber, fiber polarization controllers for controlling the polarization state of the fiber laser, waveplates for controlling linear phase delay between polarization eigenmodes of the laser, and an intra-cavity polarizer for selecting a single polarization state in the fiber laser.

11. A modelocked laser according to claim 10, wherein at least one polarization maintaining fiber is included in said cavity to minimize sensitivity of the laser performance to mechanical perturbations.

12. A modelocked laser according to claim 9, wherein said modelocking mechanism comprises non-linear polarization evolution in the fiber as a main modelocking mechanism.

13. A modelocked laser according to claim 1, wherein modelocking of said laser is initiated by inducing a cavity perturbation for self starting.

14. A modelocked laser according to claim 1, wherein said modelocking mechanism includes a saturable absorber coupled internally of or externally to said cavity, for use in self starting of modelocked laser oscillation.

15. A modelocked laser according to claim 1, wherein said modelocking mechanism comprises passive modelocking with one of Kerr-type modelocking and saturable absorber modelocking, as a main modelocking mechanism of said laser.

16. A modelocked laser according to claim 15, wherein said passive modelocking technique comprises non-linear polarization evolution.

17. A modelocked laser according to claim 1, wherein said gain medium comprises a doped optical fiber and said chirped grating comprises a chirped waveguide grating.

18. A modelocked laser according to claim 17, wherein said modelocking mechanism comprises non-linear polarization evolution in the fiber as a main modelocking mechanism.

19. A modelocked laser according to claim 1, wherein at least one polarization maintaining fiber is included in the cavity to minimize sensitivity of the laser performance to mechanical perturbations.

20. A modelocked laser according to claim 1, further comprising a plurality of wavelength tuning means for controlling intra-cavity loss and polarization state, to obtain modelocking at a plurality of wavelengths simultaneously.

21. A modelocked laser according to claim 1, wherein said laser is a modelocked Figure Eight laser including a plurality of polarization controllers.

22. A modelocked laser according to claim 21, wherein said gain medium is coupled to a nonreciprocal linear phase shifter arranged within said cavity for modelocking optimization.

23. A modelocked laser according to claim 1, wherein said modelocking mechanism includes an active modelocker coupled to a source for external timing.

24. A modelocked laser according to claim 23, wherein said active modelocker is one of an electro-optic and acousto-optic modulator.

25. A modelocked laser according to claim 1, wherein a pair of chirped gratings are arranged in said cavity, said gratings having respectively separated reflection profiles, for promoting modelocked operation of said laser at two wavelengths simultaneously.