Phase Conjugate Laser Optics

Chapter 5.3.4.4 - Second harmonic conversion

5.3.4.4   Second harmonic conversion   The high-beam-quality, high-energy
output from the phase conjugated laser system is ideally suited for harmonic
frequency conversion. The frequency doubler design philosophy used for this
system is best summarized by “less is better.” This extends to the choice of the
doubler material itself, any required auxiliary optics, and any supporting mechanical
hardware. As applied to the output of a slab laser, this means determining if efficient
conversion is possible without any beam-shaping optics intervening between the
amplifier output and the frequency converter. The nonlinear material parameters that
were evaluated with this consideration included: the nonlinear coefficient, the
optical damage threshold, the intrinsic absorption at the fundamental and the second
harmonic wavelengths, and the sensitivity of the conversion efficiency to angle,
thermal distortion, and temperature. To avoid a beam-shaping optical system, KD*P
is the only material readily available in the required size and optical quality. Given
this choice, a type II KD*P doubler was designed to achieve high conversion
efficiency on both a per-pulse and average power basis using the principles outlined
by Eimerl [41]. A detailed description of the optical design of the second harmonic
converter and the optimization modeling can be found elsewhere [29].

A maximum external conversion efficiency of 82% was obtained at 21-J / pulse
input, corresponding to a peak input irradiance of 185 MW/cm2. The overall beam
shape of the 1ω output is preserved in the 2ω beam with a reduction in the beam
divergence of 2×. Operation of the doubler at an average input power of 75 W
yielded an output at the second harmonic of 60 W with no reduction from the single
shot conversion efficiency. This performance requires only a minor optimization of
the angular orientation of the crystals for steady-state operation as predicted from
the modeling. This high level of performance can only be achieved by maintaining
high beam quality under full average power operation. The second harmonic
conversion experiments were performed at an intermediate stage in the development
of the full average power amplifier system. For this reason, operation with the
doubler at the full 150-W average input power with the 15-ns laser system was not
demonstrated but would be expected to pose no problems.


5.3.5   Summary of the 15-ns high-energy laser system


We have designed and constructed an Nd:glass amplifier system incorporating an
SBS phase conjugate mirror that operates at 25–30 J / pulse with a pulse width of
15-ns FWHM and a pulse repetition frequency of 6 Hz. This results in a peak power
of 2 GW and an average output power that significantly exceeds 150 W. The
divergence of the system is measured to be 1.25 times the diffraction limit, and the
output can be frequency doubled with an efficiency of 82%. The laboratory
prototype has proven to be an extremely reliable system and has been in continuous
operation for almost 10 years at the time of this writing. Even so, its average power
and brightness performance is still unmatched for pulse energies over 10 J. It is
presently in use as a laser source for a number of experimental investigations
including high-throughput optical damage testing for the National Ignition Facility
project [6] where the output beam frequency is being tripled, providing 10 J / pulse at
351 nm for testing.

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