Abstract:
A unique method and apparatus for locking on an absolute wavelength of laser light output by a laser package by actively compensating for a change in the temperature of an etalon optical filter is disclosed. Changes in etalon response characteristics due to temperature changes are compensated for by the addition (or subtraction) of an output voltage offset to the voltage control signal sent to the Thermo-Electric Cooler (TEC) from a controller within the laser package. The voltage offset is calculated by monitoring the etalon temperature. The voltage offset value provides for active compensation of changes in the etalon temperature and effectively “readjusts” the output of the laser as if the etalon temperature itself had been readjusted.

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
   The present application is a divisional application of U.S. patent application Ser. No. 09/352,827 filed on Jul. 13, 1999 U.S. Pat. No. 6,516,010, the disclosure of which is herewith incorporated by reference in its entirety. 

   BACKGROUND OF THE INVENTION 
   1. Field of the Invention 
   The present invention relates generally to tunable lasers and other tunable optical signal sources and more particularly to a method and system for compensating for a temperature induced shift in an etalon&#39;s Fabry-Perot output characteristics relative to a channel grid on which the laser wavelength lock is to be maintained. 
   2. Description of the Related Art 
   Optical fiber communications systems provide for low loss and very high information carrying capacity. In practice, the bandwidth of optical fiber may be utilized by transmitting many distinct channels simultaneously using different carrier wavelengths. The associated technology is called wavelength division multiplexing (WDM). In a narrow band WDM system, eight, sixteen or more different wavelengths are closely spaced to increase fiber transmission capacity. 
   The wavelength bandwidth that any individual channel occupies depends on a number of factors, including the impressed information bandwidth, and margins to accommodate carrier frequency drift, carrier frequency uncertainty, and to reduce possible inter-channel cross-talk due to non-ideal filters. 
   To maximize the number of channels, lasers with stable and precise wavelength control are required to provide narrowly spaced, multiple wavelengths. However, in practice, a laser generates light over rather broad bandwidths referred to as the laser gain curve. The only longitudinal-mode discrimination in conventional Fabry-Perot lasers is provided by the gain spectrum itself. Since the laser cavity is a type of Fabry-Perot interferometer, the energy output over the gain curve is not continuous but occurs at discrete, closely spaced frequencies. The output frequencies are based upon the number of discrete longitudinal modes that are supported by the laser cavity. The longitudinal modes will occur at wavelengths such that an integral number of half wavelengths equals the distance between the mirrors of the resonator in the laser. Laser oscillation can occur only at frequencies where the laser gain curve exceeds the losses in the optical path of the resonator. In practice, the broadened laser gain curve exceeds the cavity losses over a large frequency range, on the order of 8 to 10 GHz. As noted above, there will be a number of discrete, closely spaced modes oscillating within this range. 
   Various approaches have been used to limit the oscillation of a laser to one of the competing longitudinal modes. One approach is a distributed feedback mechanism. Distributed-feedback (DFB) lasers are the most common type of communications laser. A grating integral to the laser structure limits the output to a single frequency. Another of the most common methods requires the use of a frequency selective external cavity/etalon in combination with such a laser device to detect the output wavelength at which the laser is operating and adjust the laser accordingly by varying the temperature of the laser, known as temperature tuning. Such a method allows for wavelength locking of a laser even in the event of changing ambient temperature conditions. The external cavity/etalon laser is most commonly applied to gas tube lasers but has also been applied for very narrow line width lasers such as those needed for laser gyro use. There are a number of types of etalons. In its simplest form, an etalon consists of a quartz glass plate with parallel surfaces that is placed in the laser resonator at a non-normal angle. Internal reflections give rise to interference effects which cause the etalon to behave as a frequency selective transmission filter, passing with minimum loss frequencies close to a transmission peak and rejecting by destructive interference other frequencies. In practice, the transmission peak of the etalon is set to coincide with a particular longitudinal mode resulting in single frequency operation of the laser. 
   There are problems, however, with wavelength stability of a temperature tuned laser for a long duration due to thermal problems. Both the DFB laser and external cavity/etalon lasers need to make the wavelength insensitive to temperature change. Typically, a Thermo-Electric Cooler (TEC) and thermistor inside the laser package is sufficient to stabilize wavelength. However, with current dense wavelength division multiplexing (DWDM), wavelength stabilization to parts per million control may not be possible utilizing conventional methods. For example, a wavelength shift as illustrated in  FIG. 1  can occur. As previously noted, temperature tuning of a laser&#39;s wavelength is accomplished by varying the laser chip temperature via the control current supplied to the Thermo-Electric Cooler (TEC) that the laser chip is mounted on within the laser package. As shown in  FIG. 1 , a laser package will tune the laser chip to maintain the desired maximum output power at the desired wavelength (λ desired), illustrated by point A. As the laser temperature is changed to maintain this point, it is unavoidable due to the proximity of the etalon to the TEC within the laser package that the temperature of the etalon will also change. As the etalon temperature changes, the index of refraction of the material varies and more strongly, the etalon expands or contracts, changing the effective path lengths within the material and thereby changing the interference effects. As the effective path lengths vary, the response curve of the etalon will also vary. The control system of the laser chip will temperature tune the laser chip based on the varied etalon response curve, causing the wavelength output to vary to a different wavelength (λ actual), illustrated by point B. This wavelength shift due to control system error and hysteresis can cause problems in the end system. Since the laser is initially set to deliver, to the end system in which the laser is mounted, a specified power and wavelength output, when the wavelength of the output varies it can cause disruption to the operation of the end-product system and possibly even damage the functionality of the end-product system. 
   Thus, there exists a need for a method and apparatus for stabilizing and locking on an absolute wavelength of laser light by compensating for a temperature change of the etalon in a temperature tuned laser. 
   SUMMARY OF THE INVENTION 
   The present invention provides a unique method and apparatus for locking on an absolute wavelength of laser light by actively compensating for a change in temperature of an etalon optical filter. 
   In accordance with the present invention, changes in etalon response characteristics due to temperature changes are compensated for by the addition (or subtraction) of an output voltage offset to the voltage control signal sent to the Thermo-Electric Cooler (TEC) within the laser package. These calculations can be performed by conventional analog circuitry or by digital manipulation of analog signals by a micro-controller or similar digital signal processor. The voltage offset is calculated by monitoring the etalon temperature. The voltage offset value provides for active compensation of changes in the etalon temperature and effectively “readjusts” the output of the laser as if the etalon temperature itself had been readjusted back to its initial temperature. 
   These and other advantages and features of the invention will become apparent from the following detailed description of the invention which is provided in connection with the accompanying drawings. 

   
     BRIEF DESCRIPTION OF THE DRAWINGS 
       FIG. 1  illustrates the shift in wavelength in response to a change in an etalon response curve due to a temperature change of the etalon within a laser package; 
       FIG. 2  illustrates in block diagram form a portion of a wavelength stabilized laser control system that can actively compensate for temperature changes in an etalon in accordance with a preferred embodiment of the present invention; and 
       FIGS. 3A and 3B  illustrate in flowchart form a method for actively stabilizing a laser wavelength in accordance with the present invention. 
   

   DETAILED DESCRIPTION 
   The present invention will be described as set forth in the embodiments illustrated in  FIGS. 2-3 . Other embodiments may be utilized and structural, logical or programming changes may be made without departing from the spirit or scope of the present invention. Like items are referred to by like reference numerals throughout the description. 
   In accordance with the present invention, an absolute wavelength of laser light can be locked on by actively compensating for a change in temperature of the etalon optical filter.  FIG. 2  illustrates in block diagram form a portion of a typical wavelength stabilized laser system  10 . More specifically,  FIG. 2  illustrates a control circuit for a temperature tuned laser system  10  that can actively compensate for temperature changes in an etalon in accordance with the present invention. 
   A laser chip  12  is mounted on a Thermo-Electric Cooler (TEC)  52 . A submount (not shown) between the laser chip  12  and the TEC  52  can be used if desired for thermal expansion matching. As is known in the art for temperature tuned lasers, the output of laser chip  12  can be adjusted by modifying the temperature of laser chip  12 , as a laser chip will have an output directly related to its operating temperature. Thus, by measuring the output of the laser with respect to a desired output signal, the output of the laser can be adjusted to the desired output level by changing the temperature of the laser chip. The temperature of laser chip  12  can be adjusted by varying the temperature of TEC  52 . The temperature of TEC  52  is varied based on an input signal to TEC Driver  50  from a controller  40  through a digital to analog (D/A) converter  42 . Controller  40  may include a programmable logic device, one example being a microprocessor. If a microprocessor is used, it may be any conventional general purpose single- or multi-chip microprocessor, or may be any conventional special purpose microprocessor such as a digital signal processor. Analog signal conditioning techniques may also be applied to the A/D and D/A signals. 
   Controller  40  monitors and controls the output of laser chip  12  as follows. Laser chip  12  generates a laser output  11  and a backface output  13 . The output  13  from laser chip  12  is input to an optical splitter  14  to split the output into two separate outputs  15 ,  25 . The first output  15 , hereinafter referred to as the reference path, is input to a photodetector  16 , as is known in the art, to convert the laser from an optical signal to an electrical signal. The converted electrical signal is input to an amplifier circuit  18 , which may include for example operational amplifiers  20 ,  22  and feedback impedance  24 . The output from amplifier circuit  18  is converted from an analog signal to a digital signal by analog to digital (A/D) converter  26  and input to controller  40 . 
   The second output  25 , hereinafter referred to as the etalon path, is input to an etalon filter  30  as is known in the art. The output from the etalon filter  30  is input to a second photodetector  16   a  to convert the laser from an optical signal to an electrical signal. The converted electrical signal is input to an amplifier circuit  18   a , which may include for example operational amplifiers  20   a ,  22   a  and feedback resistor  24   a . The output from amplifier circuit  18   a  is converted from an analog signal to a digital signal by A/D converter  26   a  and input to controller  40 . 
   In accordance with the present invention, the temperature of the etalon filter  30  is monitored by a thermistor  32  and input to controller  40 . The controller  40  uses the etalon path signal, i.e., the path that passes through the etalon  30 , the reference path signal, i.e., the path that is output directly from the laser chip  12  without passing through the etalon filter  30 , and the temperature measured by thermistor  32  to monitor the etalon  30  and laser chip  12  (unless a separate thermistor is also included for monitoring the laser chip as described below) to adjust the output  11  of laser chip  12  accordingly by causing TEC driver  50  to vary the temperature of TEC  52 . 
   The operation of the circuit of  FIG. 2  will be further described with reference to the flowchart of  FIGS. 3A and 3B , which illustrate a method for actively stabilizing a laser wavelength in accordance with the present invention. Referring to  FIG. 3A , in step  100 , the laser chip  12  is turned on. In step  110 , the temperature of the laser chip  12  is measured by thermistor  32  and input to controller  40 . It should be noted that in some cases, due to the typical packaging of a laser control system such as laser control system  10 , the laser chip  12  and etalon filter  30  are in such close proximity to each other that any temperature gradient between them is negligible. Therefore, the temperature of laser chip  12  and etalon filter  30  can be measured utilizing only one thermistor, such as thermistor  32 . However, laser chip  12  and etalon filter  30  may be provided with their own thermistor if desired. Once the temperature of the laser chip is determined, an approximate wavelength of the output of the laser chip  12  can be determined, since the output of the laser chip  12  is a function of its temperature. Controller  40  can then reference a look-up table to determine the necessary temperature of the laser chip  12  to output the desired wavelength as predetermined by the end product system requirements. The values in the look-up table are defined during the calibration of laser chip  12  based on the response of laser chip  12  and can be stored, for example, in a memory of controller  40 . Based on the temperature value determined from the look-up table, controller  40  will know the required temperature of laser chip  12 , determined during calibration, to cause laser chip  12  to provide the desired output. 
   It should be understood that the wavelength vs. temperature output of laser chip  12  may vary over time as laser chip  12  ages. Thus, as the laser chip  12  ages, the values in the look-up table may no longer be accurate. To overcome this problem, the look-up tables can be supplemented by controller  40 , such as for example by a “learning” algorithm, by using historical statistical data to predict and adapt to variations in the laser chip  12  as it ages. 
   In step  120 , the signals from the reference path and the etalon path are measured by controller  40 . Controller  40  then subtracts the value of the etalon path signal from the value of the reference path signal and stores this as a Difference Value. It should be noted that compensation for laser aging can be performed in real time based on statistically predicted values for the Difference Value. In step  130 , the temperature of the etalon filter is measured by thermistor  32  and stored as an Initial Value. Controller  40  then calls an etalon temperature look-up table to determine the approximate etalon temperature for the desired etalon response curve. As previously noted, the temperature of the etalon determines the expansion of the material, which determines the effective path lengths light travels within the material and changes the interference effects. Thus, during calibration of the etalon filter, it is possible to determine how the etalon will respond at different temperatures to various wavelengths, and an expected value for the given/read temperature of the etalon can be determined. Mathematically derived models that predict this behavior can also be utilized to calculate an expected value. 
   In step  140 , the Initial Value measured in step  130  is compared to the expected value from the look-up table. If the Initial Value is equal to the expected value, then in step  160  a variable called grid_offset is set to zero. If the Initial Value is not equal to the expected value, then in step  150  the value for grid-offset is adjusted accordingly, i.e., adjusted based on the difference between the Initial Value and the expected value obtained from the look-up table. It should be noted that the purpose of steps  140 - 150  is to allow the system to self-calibrate relative to the values stored in the look-up tables prior to any actual heating/cooling of the laser chip  12  via TEC  52 , although it should be noted that laser chip  12  may self-heat at turn-on. Thus, for example, if the laser system  10  is mounted in an end-product system that has an elevated ambient temperature, the laser system  10  can immediately start to compensate for the elevated ambient temperature before any actual heating of the laser chip  12  is performed by TEC  52 . 
   In step  170 , the temperature of the etalon as measured by thermistor  32  is stored by controller  40 . Referring now to  FIG. 3B , in step  180 , the Difference Value is recalculated to be the Difference Value+the value of grid_offset, and the new value for the Difference Value is output from controller  40  through D/A converter  42  to TEC driver  50 . TEC driver  50 , in response to the signal from controller  40 , i.e., the value of the adjusted Difference Value, adjusts the temperature of TEC  52 , which correspondingly adjusts the output of laser chip  12 . 
   In step  190 , the signals from the reference path and the etalon path are again measured by controller  40 . Controller  40  then determines a new value for the Difference Value using the same calculation given with respect to step  120  above. In step  200 , the temperature of the etalon is again measured by thermistor  32 . In step  210 , it is determined if the etalon temperature has changed since the previous measurement. If the etalon temperature has not changed, no compensation for a change in etalon temperature is necessary. The method returns to step  180 , where a new value for the Difference Value is calculated by adding the value of the Difference Value as calculated in step  190  and the value of grid_offset. The new value calculated for the Difference Value is then output from controller  40  to TEC driver  50  which adjusts the temperature of TEC  52  accordingly. 
   If the etalon temperature has changed, in step  220  it is determined if the temperature change is significant enough to alter the response properties of the etalon based on the accuracy desired for the system. The higher the accuracy and resolution desired, the lower the value that would represent a significant change. Thus, for example, a temperature change of only 0.5° C. might be considered significant enough in one system, while in other systems a temperature change of at least 1.5° C. is necessary to be considered significant. The value at which a temperature change is considered significant is predetermined and may be stored by controller  40 . If the temperature change is not considered significant enough, the method returns to step  180  where a new value for the Difference Value is calculated by adding the value of the Difference Value as calculated in step  190  and the value of grid_offset. The new value for the Difference Value is then output from controller  40  to TEC driver  50  which adjusts the temperature of TEC  52  accordingly. 
   If it is determined in step  220  that the temperature change is significant enough to alter the properties of the etalon filter  30 , in step  230  a value for an offset_increment_value is calculated. The value for offset_increment_value is determined by multiplying an initial_offset_increment_value by the difference of the stored etalon temperature and the most recent measured etalon temperature, i.e., offset_increment_value=initial_offset_increment_value×((stored etalon temperature)−(measured etalon temperature)). The value of the initial_offset_increment_value is predetermined based on the properties of the material being used for the etalon and its response to temperature changes. 
   In step  240 , the value for the etalon temperature measured in step  200  is stored. In step  250 , a new value for grid_offset is determined by adding the value for offset_increment_value determined in step  230  to the previous value for grid_offset. The method returns to step  180 , where a new value for Difference Value is calculated with the new value for grid_offset from step  250 . The new value for the Difference Value is then output from controller  40  to TEC driver  50  which adjusts the temperature of TEC  52  accordingly. 
   Thus, in accordance with the present invention, the temperature of the etalon is monitored and the value for grid_offset adjusted based on the temperature change of the etalon. The laser system  10  can then effectively compensate for changes in the etalon response due to a temperature change in the etalon by using the value obtained for grid_offset in the calculation of the Difference Value which is used to control the TEC  52 . By compensating for the temperature change in the etalon, laser system  10  can effectively lock on to an absolute wavelength of laser light. 
   While the invention has been described as being implemented with a laser chip  12 , it is to be understood that the invention is not so limited and may be used with any type of laser source as is known in the art, such as for example an array of lasers, a DFB laser, a distributed Bragg reflector (DBR) laser, a Fabry-Perot laser, etc. Additionally, the invention may be used with all temperature sensitive/wavelength sensitive elements, such as for example etalons, interference filters (lowpass, bandpass, and highpass), multiple grouping of filters (bandnotch), gratings, and the like. 
   Reference has been made to embodiments in describing the invention. However, additions, deletions, substitutions, or other modifications which would fall within the scope of the invention defined in the claims may be implemented by those skilled in the art and familiar with the disclosure of the invention without departing from the spirit or scope of the invention. Also, although the invention is described as implemented by a programmable controller, preferably a microprocessor running a software program, it may be implemented in hardware, software, or any combination of the two. All are deemed equivalent with respect to the operation of the invention. Accordingly, the invention is not to be considered as limited by the foregoing description, but is only limited by the scope of the appended claims.