Methods for maintaining laser performance at extreme temperatures
View Patent ↗This disclosure concerns methods for calibrating optical emitters. For example, one calibration method is employed in connection with an optical transceiver that includes a laser. A range of temperatures is defined that includes low end and high end temperatures. At a first temperature, within the range, a first bias current to the laser is adjusted until the laser generates an optical signal at a first predefined power level. At a second temperature outside the range, a second bias current to the laser is adjusted until the laser generates an optical signal at a second predefined power level. If the second temperature is greater than the high end temperature, the second predefined power level is defined as less than the first predefined power level, and if the second temperature is less than the low end temperature, the second predefined power level is defined as greater than the first predefined power level.
1. In connection with an optical transceiver that includes an optical transmitter, a method for calibrating the optical transmitter, the method comprising:
at a first temperature falling within a predefined range bounded by a low end temperature and a high end temperature where the low end temperature is less than the high end temperature, adjusting a first bias current to the optical transmitter until the optical transmitter generates an optical signal at a first predefined power level;
at a second temperature that is outside the predefined range of the first temperature, adjusting a second bias current to the optical transmitter until the optical transmitter generates an optical signal at a second predefined power level;
defining the second predefined power level to be less than the first predefined power level, if the second temperature is greater than the high end temperature of the predefined range; and
defining the second predefined power level to be greater than the first predefined power level, if the second temperature is less than the low end temperature of the predefined range.
2. The method as recited in claim 1 , wherein:
if the second temperature is greater than the high end temperature of the predefined range, the second predefined power level is defined to be less than the first predefined level in proportion to a difference between the second temperature and the high end temperature; and
if the second temperature is less than the low end temperature of the predefined range, the second predefined power level is defined to be greater than the first predefined power level in proportion to a difference between the second temperature and the low end temperature.
3. The method as recited in claim 2 , wherein the second predefined power level is defined to be less than the first predefined power level as a linearly proportional function of the difference between the second temperature and the high end temperature, if the second temperature is greater than the high end temperature.
4. The method as recited in claim 2 , wherein the second predefined power level is defined to be greater than the first predefined power level as a linearly proportional function of the difference between the second temperature and the low end temperature, if the second temperature is less than the low end temperature.
5. The method as recited in claim 1 , wherein the predefined range of the first temperature is calculated.
6. The method as recited in claim 5 , wherein calculation of the predefined range of the first temperature is based upon a value of at least one of the following characteristics of one or more optical transmitters: slope efficiency; minimum bias current; maximum bias current; minimum power level of one or more optical signals; and, maximum power level of one or more optical signals.
7. The method as recited in claim 5 , wherein calculation of the predefined range of the first temperature is based upon performance of a plurality of optical transmitters, each of which conforms with a predefined operating specification.
8. The method as recited in claim 1 , wherein the second predefined power level is calculated.
9. The method as recited in claim 8 , wherein the second predefined power level is calculated based upon a value of at least one of the following characteristics of one or more optical transmitters: slope efficiency; minimum bias current; maximum bias current; minimum power level of one or more optical signals; and, maximum power level of one or more optical signals.
10. The method as recited in claim 8 , wherein calculation of the second predefined power level is based upon performance of a plurality of optical transmitters, each of which conforms with a predefined operating specification.
11. The method as recited in claim 1 , further comprising:
determining a first current swing at the first temperature, the first current swing corresponding with optical signals having a first predefined extinction ratio; and
determining a second current swing at the second temperature, the second current swing corresponding with optical signals having a second predefined extinction ratio.
12. The method as recited in claim 11 , further comprising:
storing respective control values for the first bias current and first current swing, correlated with the first temperature, in the optical transceiver; and
storing respective control values for the second bias current and second current swing, correlated with the second temperature, in the optical transceiver.
13. The method as recited in claim 12 , further comprising:
sensing an instantaneous temperature; and
determining a bias current value and a current swing value that correspond with the instantaneous temperature, the determination of the bias current value and a current swing value being based on the respective control values for the first bias current and first current swing and the respective control values for the second bias current and second current swing.
14. In connection with an optical transceiver that includes an optical transmitter, a method for calibrating the optical transmitter, the method comprising:
defining a range of temperatures bounded by a low temperature cutoff and a high temperature cutoff;
at a first temperature between the low temperature cutoff and the high temperature cutoff, adjusting a first bias current and a first current swing of the optical transmitter until the optical transmitter generates an optical signal at a first predefined power level and at a first predefined extinction ratio;
at a second temperature outside the defined range of temperatures, adjusting a second bias current and a second current swing of the laser until the optical transmitter generates an optical signal at a second predefined power level and at a second predefined extinction ratio;
defining the second predefined power level and the second predefined extinction ratio to be greater than, respectively, the first predefined power level and the first predefined extinction ratio, in proportion to a difference between the second temperature and the low temperature cutoff, if the second temperature is less than the low temperature cutoff; and
defining the second predefined power level and the second predefined extinction ratio to be less than, respectively, the first predefined power level and the first predefined extinction ratio, in proportion to a difference between the second temperature and the high temperature cutoff, if the second temperature is greater than the high temperature cutoff.
15. The method as recited in claim 14 , wherein the low temperature cutoff and the high temperature cutoff are calculated.
16. The method as recited in claim 15 , wherein calculation of the low temperature cutoff and the high temperature cutoff is based upon a value of at least one of the following characteristics of one or more optical transmitters: slope efficiency; minimum bias current; maximum bias current; minimum power level of one or more optical signals; and, maximum power level of one or more optical signals.
17. The method as recited in claim 15 , wherein calculation of the low temperature cutoff and the high temperature cutoff is based upon performance of a plurality of optical transmitters, each of which conforms with a predefined operating specification.
18. The method as recited in claim 14 , wherein the second predefined power level and second extinction ratio are calculated.
19. The method as recited in claim 18 , wherein the calculation of the second predefined power level and second extinction ratio is based upon a value of at least one of the following characteristics of one or more optical transmitters: slope efficiency; minimum bias current; maximum bias current; minimum power level of one or more optical signals; and, maximum power level of one or more optical signals.
20. The method as recited in claim 18 , wherein calculation of the second predefined power level and second extinction ratio is based upon performance of a plurality of optical transmitters, each of which conforms with a predefined operating specification.
21. The method as recited in claim 14 , wherein the second predefined power level and the second extinction ratio are is defined to be less than the first predefined power level and the first extinction ratio, respectively, as a linearly proportional function of the difference between the second temperature and the high temperature cutoff, if the second temperature is greater than the high temperature cutoff.
22. The method as recited in claim 14 , wherein the second predefined power level and the second extinction ratio are is defined to be greater than the first predefined power level and the first extinction ratio, respectively, as a linearly proportional function of the difference between the second temperature and the low temperature cutoff, if the second temperature is less than the low temperature cutoff.
23. The method as recited in claim 14 , further comprising:
storing respective control values for the first bias current and first current swing, correlated with the first temperature, in the optical transceiver; and
storing respective control values for the second bias current and second current swing, correlated with the second temperature, in the optical transceiver.