Phase Conjugate Laser Optics

Chapter 5.3.2.2 - Relay imaging

5.3.2.2   Relay imaging   Optimal extraction efficiency from a zigzag slab solid-
state gain medium requires the amplification of a near-top-hat spatial beam profile.
However, the high-aspect-ratio rectangular slab aperture combined with this spatial
profile results in a beam with poor near-field propagation characteristics, particularly
in the presence of thermally induced phase aberrations in the solid-state amplifier.
For this reason, the architecture presented here uses a 1:1 relay imaging telescope
inside of the regenerative amplifier ring which re-images each plane inside the
zigzag slab back onto itself, preserving uniform irradiance spatial profiles in the
amplifier for multiple ring passes. A significant part of the design of this system is
the use of a double-pass relay telescope as illustrated in Fig. 5.5. The telescope
consists simply of two lenses mounted with a confocal spacing as pressure windows
on a vacuum chamber. The counterpropagating beams pass through the lenses offset


Figure 5.5. A schematic diagram of the regenerative amplifier geometry incorporating an SBS phase conjugate mirror. In the original optical layout, without SBS phase conjugation, the Pockels cell was placed inside the ring at the position of the 908 quartz rotator and the output emerged on the beam path that is shown to enter the SBS cells.


from the optical axis, thereby allowing two separate optical paths through the
telescope.

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