Laser source with coherent beam recombination
A laser source is disclosed with coherent recombination of N spatial monomode laser beams having N phase shifters controlled by a phase-lock device ( 3 ). The phase-lock device has an optical device ( 30 ) capable of taking at least a portion of each of the N beams. The optical device has an optical element ( 32 ) capable of applying a phase deformation, and at least one matrix (M 1 ) of detectors capable of detecting a first image (im) of a wave surface corresponding to the N beams. The matrix (M 1 ) of detectors also detects a second image (im d ) deformed by the optical element ( 32 ). Processing means ( 31 ) are provided for processing the first and second images. The processing means are configured so as to measure the phase pistons between on the sub-pupils (sp j ) corresponding to the N beams and to apply phase corrections c(φ) to each of the N beams, by means of said N phase shifters so as to minimize the phase pistons.
1. A laser source with coherent recombination of N spatial monomode laser beams, comprising N phase shifters controlled by a phase-lock device, said phase-lock device comprising:
an optical device comprising means for taking at least a portion of each of said N beams, said optical device comprising an optical element for applying a phase deformation, and at least one matrix of detectors for detecting a first image of a wave surface corresponding to said N beams, and a second image deformed by said optical element; and
processing means for processing said first and second images, said processing means comprising means for measuring the phase pistons between the sub-pupils corresponding to said N beams and for applying phase corrections to each of the N beams, by means of said N phase shifters so as to minimize said phase pistons, in order to deliver an optimized recombined laser beam as output.
2. The laser source as claimed in claim 1 , wherein said processing means are configured so as furthermore to measure phase tilts between the sub-pupils and to apply phase corrections to each of the N beams, by means of said N phase shifters so as to minimize said phase pistons.
3. The laser source as claimed in claim 1 , wherein the optical deforming element is an element for defocusing by a known distance.
4. The laser source as claimed in claim 1 , wherein said processing means apply a least-squares phase-piston minimization function.
5. The laser source as claimed in claim 1 , comprising N gain media delivering said N laser beams as output.
6. The laser source as claimed in claim 5 , wherein said gain media are fiber amplifiers.
7. The laser source as claimed in claim 1 , wherein said processing means are capable of impressing on the output beam a wave surface profile approximated by phase pistons juxtaposed with said phase corrections.
8. The laser source as claimed in claim 7 , wherein said profile is a phase ramp.
9. The laser source as claimed in claim 7 , wherein said profile is a phase function for precorrecting the known perturbations of the recombined beam.
10. The laser source as claimed in claim 7 , comprising a two-dimensional array of gain media, wherein said profile is a phase function defined so as to focus the recombined beam into a spot of specified shape.
11. An optronic beam scanning system, comprising
a laser source with coherent recombination of N spatial monomode laser beams, comprising N phase shifters controlled by a phase-lock device ( 3 ), characterized in that said phase-lock device comprising:
an optical device ( 30 ) comprising means for taking at least a portion of each of said N beams, said optical device comprising an optical element ( 32 ) for applying a phase deformation, and at least one matrix (M 1 ) of detectors for detecting a first image (im) of a wave surface corresponding to said N beams, and a second mane (im d ) deformed by sad optical element ( 32 ); and
processing means ( 31 ) for processing said first and second images, said processing means comprising means for measuring the phase pistons between the sub-pupils (sp j ) corresponding to said N beams and for applying phase corrections c(φ) to each of the N beams, by means of said N phase shifters so as to minimize said phase pistons, in order to deliver an optimized recombined laser beam as output;
wherein said processing means are capable of impressing on the output beam a wave surface profile approximated by phase pistons juxtaposed with said phase corrections, wherein said profile is a phase ramp.
12. A free-space telecommunication system, comprising a laser source with coherent recombination of N spatial monomode laser beams, comprising N phase shifters controlled by a phase-lock device, said phase-lock device comprising:
an optical device comprising means for taking at least a portion of each of said N beams, said optical device comprising an optical element for applying a phase deformation, and at least one matrix of detectors for detecting a first image of a wave surface corresponding to said N beams, and a second image deformed by said optical element; and
processing means for processing said first and second images, said processing means comprising means for measuring the phase pistons between the sub-pupils corresponding to said N beams and for applying phase corrections to each of the N beams, by means of said N phase shifters so as to minimize said phase pistons, in order to deliver an optimized recombined laser beam as output;
wherein said processing means are capable of impressing on the output beam (f R ) a wave surface profile approximated by phase pistons juxtaposed with said phase corrections; wherein said profile is a phase function for precorrecting the known perturbations of the recombined beam.
13. The laser source as claimed in claim 2 , wherein the optical deforming element is an element for defocusing by a known distance.
14. The laser source as claimed in claim 2 , wherein said processing means are capable of impressing on the output beam a wave surface profile approximated by phase pistons juxtaposed with said phase corrections.
15. The laser source as claimed in claim 3 , wherein said processing means are capable of impressing on the output beam a wave surface profile approximated by phase pistons juxtaposed with said phase corrections.
16. The laser source as claimed in claim 4 , wherein said processing means are capable of impressing on the output beam a wave surface profile approximated by phase pistons juxtaposed with said phase corrections.
17. The laser source as claimed in claim 5 , wherein said processing means are capable of impressing on the output beam a wave surface profile approximated by phase pistons juxtaposed with said phase corrections.
18. The laser source as claimed in claim 6 , wherein said processing means are capable of impressing on the output beam a wave surface profile approximated by phase pistons juxtaposed with said phase corrections.
19. The laser source as claimed in claim 13 , wherein said profile is a phase function for precorrecting the known perturbations of the recombined beam.
20. The laser source as claimed in claim 13 , comprising a two-dimensional array of gain media, wherein said profile is a phase function defined so as to focus the recombined beam into a spot of specified shape.