Actively stabilized systems for the generation of ultrashort optical pulses

• US 20060056480A1
• Filed: 09/15/2005
• Published: 03/16/2006
• Est. Priority Date: 09/15/2004
• Status: Abandoned Application

• Current Assignee: Raydiance, Inc. (Coherent Corp.)
• Original Assignee: Raydiance, Inc. (Coherent Corp.)
• Inventors: Mielke, Michael Marshall, Yilmaz, Ismail Tolga, Farley, Mark, Goldman, David
• Application Number:
  US11/229,302
• Publication Number:
  US 20060056480A1
• Time in Patent Office: Days
• US Class Current: 372/94
• CPC Class Codes: H01S 3/06791 Fibre ring lasers fibre laser gyrometers G01C19/72
• CPC Class Codes: H01S 3/107 using electro-optic devices, e.g. exhibiting Pockels or Kerr effect H01S3/1061, H01S3/1063, H01S3/1065 take precedence
• CPC Class Codes: H01S 3/1109 Active mode locking
• CPC Class Codes: H01S 3/1121 Harmonically mode locking lasers, e.g. modulation frequency equals multiple integers or a fraction of the resonator roundtrip time
• CPC Class Codes: H01S 3/136 by controlling devices placed within the cavity

Abstract

A system and method for generating an optical laser pulse train of constant ultrashort pulse duration and low timing jitter in a fiber ring laser system (resonator) while keeping the laser resonator resilient to environmental conditions like temperature, humidity and pressure. The laser resonator may be actively mode-locked with a periodic electrically driven modulation at a specific frequency that corresponds to the inverse of the transit time inside the resonator. The optical pulse train quality may be monitored in real time, and the frequency of the modulation may be dynamically tuned in real time to compensate for resonator length changes due to changes in the environmental conditions.

Claims

1. A stable seed laser ring system for producing a plurality of ultrashort optical pulses, comprising:

a ring including a source for generating optical pulses, a modulator having an input for controlling the length of the optical pulses generated by the source, and an optical pulse sampler for sampling the optical pulses; and

a feedback loop coupled to the optical pulse sampler, the feedback loop including an optical detector for detecting changes in the optical pulses due to changes in the environment and a controller for varying the input to the modulator in response to the environmental changes such that the optical pulses remain significantly unaffected by such changes.

2. The system of claim 1 wherein the controller for varying the input to the modulator further comprises:

an electrical pulse generator; and

a frequency controller for varying the frequency of the pulses generated by the electrical pulse generator.

3. The system of claim 2 wherein the electrical pulse generator produces a square wave having a magnitude sufficient to transition the modulator from opaque to transparent to opaque.

4. The system of claim 2 wherein the electrical pulse generator produces a square wave having a magnitude of about 2 times the V_τ

of the modulator.

5. The system of claim 3 wherein the frequency controller for varying the frequency of the pulses generated by the electrical pulse generator further comprises circuitry for varying the frequency of the square wave.

6. The system of claim 2 wherein the frequency controller for varying the frequency generated by the electrical pulse generator further comprises circuitry for varying the time between pulses.

7. The system of claim 1 wherein the optical pulse sampler for sampling the optical pulses further comprises an optical tap for removing the pulses from the ring.

8. The system of claim 1 wherein the optical detector comprises a two-photon absorption detector.

9. The system of claim 1 wherein the optical detector comprises an optical power monitor.

10. The system of claim 1 wherein the optical detector comprises a spectrum analyzer.

11. The system of claim 1 wherein the modulator comprises an electro-optic modulator.

12. A method of producing a plurality of ultrashort optical pulses in a laser ring system, comprising:

generating a plurality of optical pulses by self-oscillation of an optical amplifier coupled in a ring to an electrically driven electro-optic modulator, in which the length of the pulses is determined by the period during which the modulator is in a transparent state;

sampling the optical pulses in the ring;

detecting changes in the optical pulses due to changes in the environment; and

adjusting the electrical signal to the modulator in response to the sampled pulses to compensate for any environmental changes such that the optical pulses in the ring remain significantly unaffected by such changes.

13. The method of claim 12 further comprising driving the modulator with a square wave, and wherein adjusting the electrical signal to the modulator further comprises changing the frequency of the square wave.

14. The method of claim 13 in which the magnitude of the square wave is about 2 times the V_τ

of the modulator.

15. The method of claim 13 in which adjusting the electrical signal to the modulator further comprises adjusting the frequency of the square wave to a frequency at which the ring is in resonance.

16. A method of producing a plurality of ultrashort optical pulses in a laser ring system, comprising:

generating laser light with a source;

inputting the generated laser light to an electrically driven electro-optic modulator to result in modulated light;

returning the modulated light to the source to establish the ring;

supplying a varying electrical signal to the modulator such that the modulator alternates between a transparent state and an opaque state and outputs optical pulses during the transparent state;

sampling the output optical pulses;

detecting changes in the optical pulses due to changes in the environment; and

adjusting the frequency of the electrical signal to the modulator in response to the sampled optical pulses to compensate for any environmental changes such that the optical pulses remain significantly unaffected by such changes.

17. The method of claim 16 wherein supplying a varying electrical signal to the modulator comprises supplying a square wave to the modulator.

18. The method of claim 17 wherein the square wave has a magnitude greater than V_τ

which is sufficient to transition the modulator from opaque to transparent to opaque.

19. The method of claim 17 wherein the square wave has a magnitude of about 2 times the V_τ

of the modulator.

20. The method of claim 16 wherein adjusting the frequency of the electrical signal to the modulator comprises adjusting the frequency of the electrical signal to a frequency at which the ring is in resonance.

21. The method of claim 17 wherein the square wave has a rise time of less than approximately 400 ps.

22. The method of claim 18 wherein the transition through V_τ

of the modulator has a jitter of less than approximately 20 ps.

23. The method of claim 16 wherein supplying a varying electrical signal to the modulator further comprises supplying a pulse having a substantially trapezoidal shape and a rise time of less than approximately 400 ps to the modulator.