Phase Conjugate Laser Optics

Chapter 5.3.2.4 - Operation with an SBS phase conjugator

5.3.2.4   Operation with an SBS phase conjugator   By replacing the
Pockels cell in the regenerative amplifier ring with a 90o quartz rotator as depicted in
Fig. 5.5, an injected pulse from the oscillator makes two revolutions through the
ring, for a total of four gain passes, before it is reflected by the polarizing beam
splitter. This reflected beam, formerly the output beam in the unidirectional
configuration, is now directed into an SBS phase conjugation cell. The wavefront-
reversed return from the conjugator retraces the two ring passes, accumulating four
more gain passes, before it is again reflected out of the ring. The high-power pulse
now retraces the input beam path and must be isolated from the oscillator. This is
accomplished by placing the Pockels cell removed from the ring into the input beam
as illustrated in Fig. 5.5. The λ/2 voltage is applied to the Pockels cell as the injected
seed pulse is transmitted into the ring, canceling its passive 90o rotation. During the
following four ring transit times, the Pockels cell voltage is switched back to zero so
that the high-energy output pulse experiences a 90o rotation and is transmitted
through the input polarizing beam splitter.

The most important advantage of operating the regenerative amplifier system
with an SBS mirror lies, of course, in its wavefront reversal properties. As the input
beam makes its first four passes through the amplifier, it accumulates wavefront
phase errors due to thermal aberrations in the solid-state amplifier slab as well as to
residual optical figure errors in the other optics in the ring. The SBS cell effectively
conjugates the phase of the input beam, producing a wavefront-reversed output
Stokes beam with a small frequency shift (<5 GHz for carbon tetrachloride, CCl4).
As this output beam retraces the path of the input beam through four additional gain
passes, the phase errors cancel and the high-quality wavefront of the injected beam
is recovered in the high energy output.

However, it is important to note that there are additional very distinct advantages
to the operation of the amplifier system with the SBS phase conjugator. Eight gain
passes through the zigzag slab amplifier can be achieved using passive polarization
switching in the regenerative amplifier ring. The fact that the SBS cell provides
interstage gain isolation makes this possible since, if it were replaced with a mirror,
the small signal gain through eight consecutive gain passes would result in possible
parasitic oscillation from the small reflective losses of AR-coated optical surfaces
in the ring or in the output beam. When the Pockels cell is located inside the
regenerative amplifier ring, the length of the laser pulse to be amplified is limited to
the transit time inside the ring minus the high-voltage switching time for the Pockels
cell. Now, with passive polarization switching, this time limit is increased to be the
transit time for four ring revolutions. Longer pulses can be amplified, and the
relative timing accuracy requirement between the injected pulse and the Pockels cell
voltage pulse is greatly reduced. In fact, the replacement of the Pockels cell with a
full-aperture Faraday isolator has been shown to allow the amplification of laser
pulses of over 500 ns in duration [32], as will be described in a following section of
this chapter.

Another advantage is that the SBS phase conjugator very effectively conjugates
the first-order aberration of tilt. The combination of this tilt correction and relay
imaging greatly reduces the sensitivity of the system performance to small changes
of optical alignment in the ring. No change in output power or pointing direction
during operation is observed for large mirror misalignments in the ring, limited only
to those angular excursions that result in vignetting of the beams at the edges of the
amplifier slab.

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