Phase Conjugate Laser Optics

Chapter 5.3.3 - SBS phase conjugation with a liquid cell

5.3.3   SBS phase conjugation with a liquid cell

The basic concept of SBS phase conjugation is well understood and is described in
more detail elsewhere in this book. However, we believe that there are a number of
important considerations to be made when incorporating an SBS phase conjugate
mirror into a high-power laser system in order to accommodate the often-required
high input energies and to maintain good near- and far-field fidelity in the amplified
output.

5.3.3.1   Wavefront reversal fidelity
 As we described in the previous section,
the conclusion that good wavefront reversal fidelity in the SBS Stokes waves is
obtainable for input powers high above threshold is very significant since there are
strong motivations for operating the SBS phase conjugator with large input energies.
In a somewhat oversimplified but still useful understanding of the SBS phase
conjugation process, an input wave with a uniform irradiance spatial profile and flat
phase profile is transmitted through an aberrating medium. If this beam is then
focused into an SBS cell, the aberrated wavefront is transformed into a distorted
irradiance spatial profile in the far field. The Stokes wave is seeded from random
acoustic fluctuations in the medium and is selectively amplified by stimulated
scattering in the regions of peak irradiance, hence peak gain. The diffraction of the
resulting counterpropagating wave then produces a reversed, or phase conjugated,
wavefront at the focusing lens. Based on this description, albeit an overly simple one,
it can be reasoned that it is desirable to operate far above threshold with a highly
aberrated input beam in order for the highest frequency modes, which appear in
spatially extended distributions at focus, to reach threshold and be reversed.

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