Mode-locked laser method and apparatus

• US 20050117614A1
• Filed: 11/30/2004
• Published: 06/02/2005
• Est. Priority Date: 12/01/2003
• Status: Active Grant

• Current Assignee: Continuum Electro-Optics Incorporated
• Original Assignee: Excel/Quantronix, Inc.
• Inventors: Fu, Qiang, Rogers, Brian, Chen, Zhengyu, Hu, Wentao, Xu, Faming
• Granted Patent: US 7,079,558 B2
• Time in Patent Office: Days
• US Class Current: 372/18
• CPC Class Codes: H01S 3/08 Construction or shape of optical resonators or components thereof
• CPC Class Codes: H01S 3/08045 Single-mode emission
• CPC Class Codes: H01S 3/1068 using an acousto-optical device
• CPC Class Codes: H01S 3/1109 Active mode locking
• CPC Class Codes: H01S 3/1305 Feedback control systems
• CPC Class Codes: H01S 3/136 by controlling devices placed within the cavity
• CPC Class Codes: H01S 3/139 by controlling the mutual position or the reflecting properties of the reflectors of the cavity , e.g. by controlling the cavity length

Abstract

A method and apparatus for stabilizing the output of a mode-locked laser by monitoring the temporal behavior of the pulse train profile and controlling the laser cavity optical length and/or loss modulation frequency accordingly. A mismatch of the cavity optical length and the loss modulation frequency will yield a first characteristic noise condition on the laser beam pulse train when the optical length is too short for a given loss modulation frequency and a second, different noise condition when the optical length is too long. The laser beam is monitored and analyzed to determine which noise condition is present. The cavity optical length is adjusted accordingly by movement of one or more optical elements or by changing the index of refraction of one or more optical elements. In the alternative, or additionally, the loss modulation frequency can be adjusted to bring the laser back into mode lock.

Claims

1. A method of stabilizing a mode-locked laser comprising:

detecting a laser light generated by the mode-locked laser;

analyzing the detected laser light to determine the presence of at least one of a plurality of noise conditions; and

adjusting at least one of a cavity optical length and a loss modulation frequency of the mode-locked laser in accordance with the noise condition present.

2. The method of claim 1, wherein the cavity optical length is increased for a first noise condition and decreased for a second noise condition.

3. The method of claim 2, wherein the first noise condition is characterized by a noise amplitude that is substantially unipolar and the second noise condition is characterized by a bipolar relaxation oscillation noise amplitude.

4. The method of claim 1, wherein the cavity optical length is adjusted by moving an optical component of the mode-locked laser.

5. The method of claim 1, wherein the cavity optical length is adjusted by changing a refraction of an optical component of the mode-locked laser.

6. The method of claim 1, wherein the loss modulation frequency is increased for a first noise condition and decreased for a second noise condition.

7. The method of claim 6, wherein the first noise condition is characterized by a noise amplitude that is substantially unipolar and the second noise condition is characterized by a bipolar relaxation oscillation noise amplitude.

8. The method of claim 1, wherein analyzing the detected laser light includes counting a first number of positive noise spikes and a second number of negative noise spikes and comparing the first and second numbers.

9. The method of claim 1, comprising:

sensing a temperature of the mode-locked laser; and

determining an initial cavity optical length adjustment based on the temperature sensed.

10. A system for stabilizing a mode-locked laser comprising:

a detector, wherein the detector detects a laser light generated by the mode-locked laser;

an analyzer, wherein the analyzer analyzes the detected laser light to determine the presence of at least one of a plurality of noise conditions; and

an adjuster, wherein the adjuster adjusts at least one of a cavity optical length and a loss modulation frequency of the mode-locked laser in accordance with the noise condition present.

11. The system of claim 10, wherein the cavity optical length is increased for a first noise condition and decreased for a second noise condition.

12. The system of claim 11, wherein the first noise condition is characterized by a noise amplitude that is substantially unipolar and the second noise condition is characterized by a bipolar relaxation oscillation noise amplitude.

13. The system of claim 10, wherein the adjuster adjusts the cavity optical length by moving an optical component of the mode-locked laser.

14. The system of claim 10, wherein the adjuster adjusts the cavity optical length by changing a refraction of an optical component of the mode-locked laser.

15. The system of claim 10, wherein the adjuster increases the loss modulation frequency for a first noise condition and decreases the loss modulation frequency for a second noise condition.

16. The system of claim 15, wherein the first noise condition is characterized by a noise amplitude that is substantially unipolar and the second noise condition is characterized by a bipolar relaxation oscillation noise amplitude.

17. The system of claim 10, wherein the analyzer includes:

a first counter, wherein the first counter counts a first number of positive noise spikes;

a second counter, wherein the second counter counts a second number of negative noise spikes; and

a comparator, wherein the comparator compares the first and second numbers.

18. The system of claim 10, comprising:

a temperature sensor, wherein the temperature sensor senses a temperature of the mode-locked laser; and

means for determining an initial cavity optical length adjustment based on the temperature sensed.