Abstract

Spatial phase locking was achieved experimentally for radiation from linear arrays of 4 and 12 wide-aperture multimode semiconductor lasers. This phase locking was attained in an external cavity of 1 < L < 3 cm length with a plane mirror (R=90%) by diffractive exchange of radiation between neighbouring lasers. An analysis of all possible cavity oscillation eigenmodes (supermodes) was made for a phase-locked array of 4 coupled lasers. The output radiation of this array was characterised by a high degree of coherence (with the contrast of V=0.9). The angular width (at half-maximum) dy was 1.2 mrad for the fundamental (ν =1) and highest (ν =4) supermodes, and 0.8 mrad for the modes with ν =2 or 3, which corresponded to the diffraction limit. Full supermode selection was achieved in the 4-laser array as a result of the Talbot effect when the cavity length was L=ZT/4. The far-field distribution of the radiation was then characterised by the parameters V=0.98 and δψ = 1.2 mrad. The corresponding parameters of a phase-locked 12-laser array were V=0.93 for the axial propagation zone and δψ =0.46 mrad.

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