Mode-locked laser method and apparatus
View Patent ↗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.
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, wherein a first noise condition indicates that a cavity optical length is too short and a second noise condition indicates that a cavity optical length is too long and wherein the first and second noise conditions have different noise characteristics that are analyzed to determine which noise condition is present; 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 adjusted wherein the cavity optical length is increased for the first noise condition and decreased for the 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 the first noise condition and decreased for the 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 is configured and arranged to detect a laser light generated by the mode-locked laser;
an analyzer, wherein the analyzer is configured and arranged to analyze the detected laser light to determine the presence of at least one of a plurality of noise conditions, wherein a first noise condition indicates that a cavity optical length is too short and a second noise condition indicates that a cavity optical length is too long and wherein the first and second noise conditions have different noise characteristics, wherein the analyzer is configured and arranged to analyze the noise characteristics to determine which noise condition is present; and
an adjuster, wherein the adjuster is configured and arranged to adjust 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 system is configured and arranged so that the cavity optical length is increased for the first noise condition and decreased for the 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 is configured and arranged to adjust the cavity optical length by moving an optical component of the mode-locked laser.
14. The system of claim 10 , wherein the adjuster is configured and arranged to adjust 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 is configured and arranged to increase the loss modulation frequency for a first noise condition and is configured and arranged to decrease 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 is configured and arranged to count a first number of positive noise spikes;
a second counter, wherein the second counter is configured and arranged to count a second number of negative noise spikes; and
a comparator, wherein the comparator is configured and arranged to compare the first and second numbers.
18. The system of claim 10 , comprising:
a temperature sensor, wherein the temperature sensor is configured and arranged to sense a temperature of the mode-locked laser; and
means for determining an initial cavity optical length adjustment based on the temperature sensed.
19. The method of claim 1 , wherein the noise characteristics comprise a polarity of the noise.
20. The system of claim 10 , wherein the noise characteristics comprise a polarity of the noise.