Phase Conjugate Laser Optics

Chapter 5.3.3.3 - Relay imaging to the SBS cell

5.3.3.3   Relay imaging to the SBS cell   A highly relayed optical system, as
described in previous sections, is essential for the successful operation of a phase
conjugated amplifier system. As wavefront aberration accumulates on the laser pulse
circulating in the amplifier, the system optics must collect, relay, and deliver to the
SBS cells all components of the aberrated beam. In addition to this, we have found
that the irradiance spatial profile delivered to the SBS oscillator is also significant. It
is important that aberrations on the wavefront not be allowed to freely propagate,
producing a distorted irradiance spatial profile. The near-field reproduction in the
SBS conjugator return is observed to be poor for a strongly modulated input
irradiance profile. If the distorted phase information is lost to near-field distortion in
the beam, then this poor near-field reproduction will degrade the phase conjugation
fidelity of the SBS mirror. By image relaying the amplifier aperture to the focusing
lens of the SBS oscillator, a smooth spatial profile is presented to the phase
conjugator. Any errors in the near-field irradiance distribution in the SBS return in
the form of small amplitude modulation are then reduced by gain saturation in the
final amplifier passes.


5.3.3.4   Temporal fidelity   It is also important to operate the SBS phase
conjugator high above threshold to have high reflectivity and the best reproduction
of the temporal profile of the input pulse. The energy efficiency of the phase
conjugate mirror is determined primarily by the leading-edge portion of the input
pulse that is transmitted through the cells and lost before the SBS threshold is

Figure 5.6. (a) The experimentally measured reflected energy versus input energy for the twocell CCl4 SBS phase conjugator arrangement with 15-ns FWHMinput pulses. (b) The same data plotted as SBS reflectivity versus input energy.

reached. For this reason, maximizing the SBS efficiency also optimizes the temporal
reproduction fidelity of the input pulse. Figure 5.6 shows the reflectivity versus input
energy for the described two cell amplifier/oscillator configuration up to the
nominal operating input level of 2.5 J. The reflectivity saturates at a maximum value
of 88% beyond ~ 1 J. The insertion loss into the optical beam train is very small
with this high value of the SBS conversion efficiency, and virtually no pulse
shortening or steepening of the leading edge of the output temporal profile is
observed.

5.3.3.5   Liquid SBS medium purity   The purity of the SBS medium is crucial
with respect to minimizing both optical absorption and the possibility of optical
breakdown at the focus of the SBS oscillator. The removal of dissolved impurities
which can undesirably increase absorption can normally be accomplished by
distillation techniques. In practice, however, we have determined that in the case of
most liquid SBS media, it is sufficient to use the commercially available 99.9%
spectroscopic-grade material. However, a more challenging problem was found to
be the presence of suspended particulate impurities which, when intercepted by the
focused input beam, lead to a significantly reduced optical breakdown threshold.
The most effective way of removal of these particles has been found to be the use of
a closed-loop filtration system installed on the SBS oscillator cell. A small
centrifugal pump of stainless steel and teflon construction is used to circulate the
CCl4 through a 0.1-μm filter. Once the cell has been adequately filtered, it is not
necessary to run the circulation system during operation of the laser amplifier. After
filtration, the optical breakdown threshold for the 10- to 15-ns input pulses is
increased from ~ 40 mJ to over 1 J for the single-focused SBS cell.

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