Abstract
Our laser scheme is shown in on Fig, 1. The characteristic four-channel (C1,..,C4) property of the laser system is realized by an optical scheme with two Brillouin cells (BCs) as phase lockers, which are locked with a third BC and a phase-conjugating SBS mirror M. This scheme allows us to compensate not only for aberrations but also for beam depolarization in the laser rods.
© 1995 Optical Society of America
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