Phase Conjugate Laser Optics

Chapter 5.5.2 - Optical architecture of the phase-locked system

5.5.2   Optical architecture of the phase-locked system

The optical design of the phase-locked amplifier system is very closely related to the
500-ns system described in the previous section. Each amplifier arm performs
essentially just as for the single-channel long pulse laser. Since the pulse format goal
of 500 ns remains, the same oscillator design with the bi-exponential rise and 200-ns
FWHM is used. A second preamplifier stage consisting of a 9-mm Nd:YLF
flashlamp-pumped rod was added to boost the injected signal to 400 mJ (100 mJ for
each amplifier). Figure 5.26 illustrates the design concept in a very straightforward
and schematic way. A single oscillator beam is spatially divided into four separate
beams using simple “scraper” type mirrors at 45o. Each of these beams, as shown in
the figure, is directed through a four-pass Nd:glass zigzag amplifier. Each amplifier
box in the drawing represents an amplifier and all of the supporting multi-pass
optical components associated with it. After four passes through the amplifiers, the
four beams are brought back together, side by side, and directed into the SBS phase
conjugate mirror. Figures 5.26 and 5.27 depict this mirror as a simple single-lens
focused system for the purpose of clarity. The details of the three-pass SBS loop
phase-locking system will be described in a section to follow. After reflection from
the SBS cell, the four beams again split and follow separate paths through their
respective amplifiers and are rejoined in the output beam of the laser. Just as with the
single-channel long-pulse laser system, a permanent-magnet Faraday rotator located
in each amplifier arm isolates the high-energy output pulses from the injected input
beam.

Figure 5.27 takes on the slightly more daunting task of showing the actual beam
paths and component placements used in the phase-locked laser system. Although an
initial impression might be one of significant complexity, a careful comparison of
this optical layout to that of the single-channel system shown in Fig. 5.14 easily
reveals the direct correlation between the two designs. However, there are several
unique features to note in the four-beam system.

 

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