Phase Conjugate Laser Optics

Chapter 5.2 - High-Energy SBS Phase Conjugation

5.2   HIGH-ENERGY SBS PHASE CONJUGATION

As we began our first efforts to develop a high-average-power solid-state laser
system with an output energy of >25 J/pulse, we recognized that the practical
design of a MOPA geometry would require the SBS phase conjugate mirror to
reflect energies in the range of 1–3 J/pulse. With input pulse durations of around
15 ns, this represents up to 1000 times the SBS threshold for nonlinear media such as
carbon tetrachloride (CCl4) and high-pressure nitrogen (N2). It had been proposed
that SBS phase conjugators could be scaled to high peak powers using two-stage
amplifier-generator designs [10–12]. However, when possible, we believed that it
was desirable to employ a single-cell, simple-focused conjugator geometry operated
many times above threshold, from the standpoint of achieving high reflectivity,
accurate temporal pulse shape reproduction, and design simplicity. Even for the two-
cell design, our experience indicated that it was advantageous to operate the focused
generator cell high above threshold for optimal reversal of the high-frequency
spatial content of the beam wavefront.

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