Passively mode locked-laser and method for generating a pseudo random optical pulse train

• US 5,488,620 A
• Filed: 01/05/1995
• Issued: 01/30/1996
• Est. Priority Date: 01/05/1995
• Status: Expired due to Term

• Current Assignee: Hughes Electronics Corporation (AT&T, Inc.)
• Original Assignee: Hughes Aircraft Company (Rtx Corporation)
• Inventors: Minden, Monica L.
• Primary Examiner(s): Scott, Jr., Leon
• Application Number:
  US08/369,050
• Time in Patent Office: 390 Days
• Field of Search: 372/18, 372/19, 372/31, 372/11, 372/6, 372/23, 372/69, 372/75, 376/102, 376/29
• US Class Current: 372/18
• 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 3/09415 the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping
• CPC Class Codes: H01S 3/10046 Pulse repetition rate control H01S3/11 takes precedence
• CPC Class Codes: H01S 3/1022 by controlling the optical pumping
• 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

Abstract

A passively mode-locked laser and method for generating a coherent pseudo random pulse train is disclosed. The laser comprises an optical resonant cavity that is capable of sustaining the oscillation of a plurality of resonant modes having respective phases. A saturable absorber is positioned in the resonant cavity and has an optical intensity threshold beyond which multiple mode-locked pulses with random starting times are generated in the resonant cavity and periodically emitted by the laser. A pump injects power into the resonant cavity at a level at which the optical intensity that is incident on the saturable absorber exceeds the optical intensity threshold.

Claims

1. A passively mode-locked laser, comprising:

an optical resonant cavity that is capable of sustaining the oscillation of a plurality of resonant modes having respective phases;

a saturable absorber that is positioned in the resonant cavity, said saturable absorber having a threshold beyond which a pseudo random pulse train is generated; and

a pump that injects power into the resonant cavity at a level at which the optical intensity that is incident on the saturable absorber exceeds said threshold.

2. The passively mode-locked laser of claim 1, wherein said optical resonant cavity has a negative dispersion coefficient at said modes.

3. The passively mode-locked laser of claim 2, further comprising an optical filter that is positioned in said cavity to limit oscillation in said cavity to said modes.

4. The passively mode-locked laser of claim 1, wherein said optical resonant cavity comprises an optical fiber that is doped with an active gain medium.

5. The passively mode-locked laser of claim 4, wherein said optical fiber is a dispersion shifted optical fiber that has a negative dispersion coefficient at the resonant modes.

6. The passively mode-locked laser of claim 5, further comprising a grating that is imprinted on said fiber for limiting the oscillations in said fiber to said modes.

7. The passively mode-locked laser of claim 5, wherein one of the resonant modes is a central mode that has a wavelength of at least approximately 1.5^-6 meters.

8. The passively mode-locked laser of claim 4, wherein said saturable absorber comprises a non-linear reflector that is positioned at one end of the optical fiber, the reflectivity of said reflector increasing as the incident optical intensity increases.

9. The passively mode-locked laser of claim 8, wherein said pump is a laser diode.

10. The passively mode-locked laser of claim 1, wherein the pseudo random pulse train has a plurality of periods, further comprising a controller for controlling the level of the pumping power between a plurality of levels to select the number of randomly spaced mode-locked pulses in each of said periods.

11. A passively mode-locked laser, comprising:

an optical resonant cavity that is capable of sustaining the oscillation of a plurality of resonant modes with respective phases, said cavity having a loss mechanism that tends to distribute the laser energy over time;

a saturable absorber that is positioned in the resonant cavity and tends to concentrate the laser energy in time by forcing the modes'"'"' phases to be approximately equal, said loss mechanism and said saturable absorber combining to establish a threshold beyond which a pseudo random pulse train is produced; and

a pump that injects power into the resonant cavity at a level at which the optical intensity incident in the cavity exceeds said threshold.

12. The passively mode-locked laser of claim 11, wherein said optical resonant cavity has a negative dispersion coefficient at said modes.

13. The passively mode-locked laser of claim 12, wherein the pulse train has a plurality of periods, further comprising a controller for controlling the level of the pumping power between a plurality of levels to select the number of randomly spaced mode-locked pulses in each of said periods.

14. A passively mode-locked fiber optic laser, comprising:

a first optic fiber having first and second ends, said fiber being doped to provide an active gain medium which is capable of sustaining the oscillation of a plurality of resonant modes having respective phases;

a nonlinear reflector that is coupled to the first end of the fiber, said nonlinear reflector having a threshold beyond which a pseudo random pulse train is generated;

an optical coupler that is coupled to the second end of the fiber for input coupling optical power into said fiber and output coupling said pseudo random pulse train; and

a pumping laser diode that provides said optical power to said optical coupler at a level at which the optical intensity that is incident on the nonlinear reflector exceeds said threshold.

15. The passively mode-locked fiber optic laser of claim 14, wherein the pulse train has a plurality of periods, further comprising a controller for controlling the level of the pumping power between a plurality of levels to select the number of randomly spaced mode-locked pulses in each of said periods.

16. The passively mode-locked fiber optic laser of claim 14, further comprising a dispersion shifted optic fiber that is connected between said optic fiber and said nonlinear reflector, said dispersion shifted fiber having a negative dispersion coefficient at said modes.

17. The passively mode-locked fiber optic laser of claim 16, wherein said optic fiber and said dispersion shifted optic fiber are combined into a single dispersion shifted fiber.

18. A method for generating a pseudo random optical pulse train, comprising:

providing an active gain medium that is capable of emitting light at discrete frequencies;

amplifying the light at a plurality of modes;

distributing the optical energy over time as a function of optical intensity;

concentrating the optical energy in time as a function of optical intensity to establish a threshold beyond which said pseudo random pulse train is produced; and

pumping said active gain medium with a sufficient amount of power so that the optical intensity exceeds said threshold.

19. The method of claim 18, wherein said pulse train has a plurality of periods, further comprising controlling the amount of pumping power to select the number of randomly spaced mode-locked pulses in each of said periods.