Phase Conjugate Laser Optics

Chapter 5.5.2.2 - The four-beam optical transport system

5.5.2.2   The four-beam optical transport system   The goal of the design of
the optical beam train for the phase-locked amplifier system was to use shared
optical components, as possible, to reduce the parts count and overall complexity of
the system. The 1:1 image-relay telescopes inside the multipass regenerative
amplifier train as well as the polarizing beam splitters that couple the beams in and
out of the ring are shared by all four extraction beams. As can be seen in Fig. 5.27, it
is only at the amplifier end of the telescopes that individual beams are picked off and
directed through separate zigzag amplifiers. The output beam from the oscillator/
preamplifier injection system is expanded to a 30-mm round beam before it passes
through a 45-mm clear-aperture permanent-magnet Faraday rotator. The beam is
then anamorphically expanded by a factor of four in the horizontal dimension using



a cylindrical telescope. A set of large-aperture polarizers is used to inject this
30 × 120-mm input beam into the amplifier beam train in s-polarization. A
25 × 100-mm mask and a set of high reflecting mirrors on the amplifier bench are
used to divide the beam into four 25 × 25-mm2 beamlets that are then directed into
individual 45-mm Faraday rotators. An anamorphic image relay telescope of the
same design used in the single-beam amplifier system (Fig. 5.14) then reshapes each
of these square beamlets to the 7 × 120-mm2 extraction beams for the Nd:glass
zigzag amplifiers. After four amplifier passes, the beams are then coupled out of the
ring on shared optics and directed to the SBS phase conjugate mirror. A cylindrical
down collimating telescope reduces the beam sizes to 7 × 12 mm2 for introduction
into the SBS system. Just as with our previous designs, the four Stokes beams
generated by the SBS mirror retrace their paths, accumulating an additional four
gain passes. The high-energy output beams are coupled out in p-polarization through
the injection polarizer and propagate to the second harmonic converter.

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