Phase Conjugate Laser Optics

Chapter 5.5.3.4 - Phase-locked pointing stability

5.5.3.4   Phase-locked pointing stability   The mechanical isolation of the
injection laser system from the amplifier optical bench was expected to provide
significantly increased pointing stability in the 100-J / pulse phase locked laser system
as compared to that measured for the 30-J / pulse long-pulse laser (Fig. 5.24). In the
vertical dimension, orthogonal to the phase-locking plane, this improvement was
successfully realized, as shown in Fig. 5.38. The pointing jitter, normalized against
beam dimensions, was decreased by a factor of two over the single-beam laser system,
with an RMS variation of only 2% of 2λ / D at 1053 nm. However, in the horizontal
dimension, a new source of beam pointing jitter was introduced in the phase-locked
laser. Very small shot-to-shot variation in the locking accuracy (beamlet to beamlet
piston phase variations) was found to introduce additional pointing fluctuation. While
this variation does not significantly degrade the Strehl from pulse to pulse, the RMS
pointing stability is reduced by 2× in the phase-locking dimension as compared to the


Figure 5.36. The far-field divergence profile for the near field distribution shown in Fig. 5.35 measured at 1 Hz. The divergence is increased to 1.25 times the diffraction limit by uncorrected aberrations introduced in the second harmonic converter and final anamorphic telescope.

vertical dimension. The measured pointing stability is nevertheless notable for a high-
energy, high-average-power pulsed laser. The 2σ fluctuation of 4.4 μrad in the
horizontal, phase-locking dimension for the phase-locked array is only 2.6% of the 2λ /
D diameter of a single beamlet at 1053 nm.

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