Multi-element Fabry-Perot etalon interferometer for direct detection lidar
A number of etalons together are used to extract the velocity, density and temperature of a scattering medium, such as the atmosphere. An optical air data sensor system incorporates the structure and operation for outputting laser light at a volume of air so as to be scattered by molecules and aerosols in the air volume being scanned; receiving the scattered laser light via a collecting optics assembly; splitting the received scattered laser light from the input optical fiber into a plurality of scattered light emissions; collimating each of the plurality of scattered light emissions; inputting the plurality of collimated light emissions into corresponding ones of a plurality of Fabry-Perot etalons; and imaging each of the plurality of collimated light emissions from the plurality of Fabry-Perot onto corresponding ones of a plurality of non-imaging detectors.
1. An optical air data sensor system, comprising:
a laser source for outputting laser light to be scattered by molecules and aerosols in the atmosphere being scanned;
a collecting optics assembly for receiving the scattered laser light including an input optical fiber; and
an interferometer including collimating optics configured to collimate inputted scattered laser light from the input optical fiber into a collimated light emission, at least three beam splitters operatively positioned to split the collimated light emission into at least three collimated light emissions, at least three Fabry-Perot etalons each operatively configured to receive a corresponding one of the at least three collimated light emissions, and at least three imaging optics operatively configured to receive a corresponding one of plurality of collimated light emissions from the at least three Fabry-Perot etalons and to image the plurality of collimated light emissions onto corresponding ones of at least three non-imaging detectors.
2. An optical air data sensor system according to claim 1 , wherein each of the at least three Fabry-Perot etalons is configured with a center frequency different from center frequencies of all others of the plurality of Fabry-Perot etalons.
3. An optical air data sensor system according to claim 1 , wherein the interferometer further includes collimating optics configured to collimate the inputted scattered laser light from the input optical fiber into a collimated light emission, at least ten beam splitters operatively positioned to split the collimated light emission into at least ten collimated light emissions, at least ten Fabry-Perot etalons each operatively configured to receive a corresponding one of the at least ten collimated light emissions, and a plurality of imaging optics operatively configured to receive a corresponding one of plurality of collimated light emissions from the at least ten Fabry-Perot etalons and to image the plurality of collimated light emissions onto corresponding ones of at least ten non-imaging detectors.
4. A method for optically sensing an air volume, comprising the steps of:
providing an interferometer that includes collimating optics configured to collimate inputted scattered laser light into a collimated light emission, at least three beam splitters operatively positioned to split the collimated light emmission into a plurality of collimated light emissions, at least three Fabry-Perot etalons each operatively configured to receive the collimated light emissions, and at least three imaging optics operatively configured to receive corresponding ones of the collimated light emissions from the at least three Fabry-Perot etalons and to image the collimated light emissions onto corresponding ones of at least three non-imaging detectors;
outputting laser light at a volume of air so as to be scattered by molecules and aerosols in the air volume being scanned;
receiving the scattered laser light so as to be inputted into the interferometer;
collimating the received scattered laser light via the collimating optics into a collimated light emission;
splitting the collimated light emmission into a plurality of collimated light emissions;
in putting the plurality of collimated light emissions into corresponding ones of the at least three Fabry-Perot etalons; and
imaging each of the plurality of collimated light emissions from the at least three Fabry-Perot etalons onto corresponding ones of the at least three non-imaging detectors.
5. A method according to claim 4 , further comprising the step of:
configuring each of the at least three Fabry-Perot etalons is configured with a center frequency different from center frequencies of a II others of the plurality of Fabry-Perot etalons.
6. A method according to claim 4 , further comprising the steps of:
providing an interferometer that includes collimating optics configured to collimate inputted scattered laser light into a collimated light emission, at least ten beam splitters operatively positioned to split the collimated light emmission into a plurality of collimated light emissions, at least ten Fabry-Perot eta Ions each operatively configured to receive the collimated light emissions, and at least ten imaging optics operatively configured to receive corresponding ones of the collimated light emissions from the at least ten Fabry-Perot etalons and to image the collimated light emissions onto corresponding ones of at least ten non-imaging detectors;
splitting the received scattered laser light from the input optical fiber into the plurality of scattered light emissions via the at least ten beam splitters;
in putting the plurality of collimated light emissions into corresponding ones of the at least ten Fabry-Perot etalons; and
imaging each of the plurality of collimated light emissions from the at least ten Fabry-Perot etalons onto corresponding ones of the at least ten non-imaging detectors.