# US 2014/0369368 A1 · Thermal Locker > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 2014/0369368 A1 - Document ID: US20140369368A1 - Status: Published application - Kind: A1 - Application number: 13/920,904 - Filed: 2013-06-18 - Published: 2014-12-18 - Earliest claimed: 2013-06-18 - Assignees: Oclaro, Inc. - Applicants: Oclaro, Inc. - Inventors: Andrew Cannon Carter; Barrie Flintham; Adrian Perrin Janssen; Colin Smith - Web page: https://patentgrep.com/patent/US20140369368A1 ## CPC - H01S 3/10: Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating - H01S 5/02325: Mechanically integrated components on mount members or optical micro-benches - H01S 3/107: using electro-optic devices, e.g. exhibiting Pockels or Kerr effect {(H01S3/1061, H01S3/1063, H01S3/1065 take precedence)} - H01S 3/1106: Mode locking - H01S 3/1305: {Feedback control systems} - H01S 5/0612: {controlled by temperature} - H01S 5/0617: {using memorised or pre-programmed laser characteristics} - H01S 5/06804: {by monitoring an external parameter, e.g. temperature} - H01S 5/0687: Stabilising the frequency of the laser - H01S: DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL ## Abstract An assembly includes an etalon assembly for dynamically locking a frequency of an optical beam to a set frequency, the etalon assembly being external to a laser source assembly that outputs the optical beam. The etalon assembly includes an etalon that receives the optical beam and generates via interference effects a transmission beam, the etalon having a thermal tuning range greater than one half of a free spectral range of the etalon. The etalon assembly also includes an etalon heater mounted to the etalon such that the etalon heater is configured to adjust the temperature of the etalon. The assembly includes a controller configured to retrieve calibration data based on the set frequency, calculate a set temperature for the etalon using a thermal tuning algorithm and the calibration data, and control the etalon heater such that the etalon has a temperature equal to the calculated set temperature. ## Claims ### Claim 1 An assembly comprising: an etalon assembly for dynamically locking a frequency of an optical beam to a set frequency, the set frequency being selected from any frequency within a frequency band, the etalon assembly being external to a laser source assembly that outputs the optical beam, the etalon assembly comprising: an etalon that receives the optical beam and generates via interference effects a transmission beam, wherein the transmission beam is a periodic function that depends on the temperature of the etalon, and a thermal tuning range of the etalon is greater than one half of a free spectral range of the etalon, and an etalon heater mounted to the etalon such that the etalon heater is configured to adjust the temperature of the etalon; and a controller configured to: retrieve calibration data based on the set frequency, calculate a set temperature for the etalon using a thermal tuning algorithm and the calibration data, and control the etalon heater such that the etalon has a temperature equal to the calculated set temperature. ### Claim 2 (depends on 1) The assembly of claim 1, wherein the etalon has a thermal optic coefficient within the range 2 to 4 GHz/C, and a thermal conductivity greater than 10 W/m·K. ### Claim 3 (depends on 2) The assembly of claim 2, wherein the etalon is a single crystal of yttrium aluminum garnet. ### Claim 4 (depends on 1) The assembly of claim 1, wherein the etalon assembly further comprises a thermally conductive shroud that surrounds a portion of etalon and is in contact with the etalon heater, and the shape of the shroud is designed to provide a uniform thermal profile to the etalon. ### Claim 5 (depends on 1) The assembly of claim 1, wherein the etalon heater is a resistive heater. ### Claim 6 (depends on 5) The assembly of claim 5, wherein the etalon assembly further comprises: an insulator that is mounted to the bottom of the etalon heater and is mounted to a submount at a temperature different than the etalon heater in a manner to insulate the etalon heater from the submount, the insulator comprising at least one air gap between a portion of the insulator and the etalon heater. ### Claim 7 A method comprising: receiving a set frequency, the set frequency being selected from any frequency within a frequency band; retrieving calibration data based on the set frequency; calculating a set temperature for an etalon using a thermal tuning algorithm and the calibration data, wherein a thermal tuning range of the etalon is greater than one half of a free spectral range of the etalon; and controlling the etalon assembly such that the etalon has a temperature equal to the calculated set temperature to dynamically lock a frequency of an optical beam to the set frequency. ### Claim 8 (depends on 7) The method of claim 7, wherein retrieving calibration data based on the set frequency comprises: locating a calibration point, of a plurality of calibration points, nearest the set frequency, wherein the plurality of calibration points are distributed across a frequency band divided up into segments that each have a bandwidth at least as large as the thermal tuning range of the etalon, and at least one calibration point is located within each segment; and retrieving the located calibration point and an associated calibration temperature (Tnom). ### Claim 9 (depends on 8) The method of claim 8, wherein the thermal tuning algorithm comprises: υi,j=υi,0+dυ/dT(Tnom−Tj) where dυ/dT is the etalon frequency change with temperature, υi,0 is the calibration point, Tj is the temperature of the etalon, and υi,j is the set frequency. ### Claim 10 (depends on 8) The method of claim 8, wherein the thermal tuning algorithm comprises: υ i , j = υ i , 0 +  υ ′  T  ( T nom - T j ) where υ is frequency,  υ ′  T is a function of frequency, υi,0 is the calibration point, Tj is the temperature of the etalon, and υi,j is the set frequency. ### Claim 11 (depends on 8) The method of claim 8, wherein the thermal tuning algorithm comprises: υ i , j = υ i , 0 +  υ ′  T  ( T nom - T j )  ( 1 - δ ) where υ is frequency,  υ ′  T function of frequency, υi,0 is the calibration point, Tj is the temperature of the etalon, υi,j is the set frequency, and where δ is a temperature offset correction factor. ### Claim 12 (depends on 8) The method of claim 8, wherein the frequency band is the C-band. ### Claim 13 An assembly comprising: a laser source assembly that produces an output beam at an initial frequency, where the initial frequency is dependent on one or more laser parameters; a redirection assembly that splits an output beam into a reference beam and a redirected beam; a reference detector that monitors the reference beam, producing a reference signal proportional to the optical intensity of the reference beam; an etalon assembly comprising: an etalon that receives the redirected beam and generates via interference effects a transmission beam, the etalon being a single crystal, and the transmission beam being dependent on a temperature of the etalon, and an etalon heater that adjusts the temperature of the etalon; and a transmission detector that monitors the transmission beam, producing a transmission signal proportional to the optical intensity of the transmission beam; and a controller configured to: control the laser source assembly in accordance with the one or more laser parameter settings, such that the initial frequency is at or near a set frequency the set frequency being selected from any frequency within a frequency band, determine a temperature of the etalon that corresponds to the set frequency, control the etalon heater such that the etalon is at the determined temperature, calculate a lock ratio using the reference signal and the transmitted signal, and adjust one or more of the one or more laser parameters until the lock ratio corresponds to a calibrated lock ratio for the set frequency. ### Claim 14 (depends on 13) The assembly of claim 13, wherein the etalon has a thermal optic coefficient within the range 2 to 4 GHz/C, and a thermal conductivity greater than 10 W/m·K. ### Claim 15 (depends on 14) The assembly of claim 14, wherein the etalon is a single crystal of yttrium aluminum garnet. ### Claim 16 (depends on 13) The assembly of claim 13, wherein the one or more laser parameters include a drive current for the laser source assembly and a laser source assembly temperature value. ### Claim 17 (depends on 16) The assembly of claim 16, further comprising: a thermally conductive submount comprising a first surface and a second surface opposite the first surface, wherein the laser source assembly is mounted to the first surface of the submount; and a temperature regulator that is mounted to the second surface of the submount, and is configured to adjust the submount to the laser source assembly temperature value. ### Claim 18 (depends on 13) The assembly of claim 13, wherein the controller is further configured to: receive a second set frequency that is different from the first set frequency; control the laser source assembly in accordance with the one or more laser parameter settings, such that the initial frequency is at or near the different set frequency; determine a second temperature of the etalon that corresponds to the different set frequency; control the etalon heater such that the etalon is at the second temperature; calculate a second lock ratio using the reference signal and the transmitted signal; and adjust one or more of the one or more laser parameters until the lock ratio corresponds to a calibrated lock ratio for the second set frequency. ### Claim 19 (depends on 13) The assembly of claim 13, wherein the redirection assembly comprises: a first reflecting surface configured to change the direction of a portion of the output beam by 90 degrees such that it is propagating vertically, and transmit a remaining portion of the output beam toward the reference monitor as the reference beam; and a second reflecting surface, vertically offset from the first reflecting surface, configured to redirect the beam in a direction parallel to, and vertically offset from the output beam, to create the redirected beam. ### Claim 20 (depends on 19) The assembly of claim 19, wherein the redirection assembly comprises: a linear polarizer positioned to polarize the output beam prior to it being incident on the first reflecting surface; and a quarter-wave plate positioned to rotate the polarization of the redirected beam by 45 degrees and rotate a back reflection by an additional 45 degrees such that the rotated back reflection is orthogonal to the orientation of the linear polarizer.