Phase Conjugate Laser Optics

Chapter 5.3.2.5 - Single-frequency oscillator

5.3.2.5   Single-frequency oscillator   The 1053-nm transition in Nd:YLF
closely matches the fluorescence curve peak in the Nd-doped phosphate glass used
in this amplifier system. It is desirable to have a single-frequency oscillator input
pulse both for generating reproducible smooth temporal input profiles without
modulation from multilongitudinal modes and for achieving the best wavefront
reversal fidelity in the SBS phase conjugator [33, 34]. Although single longitudinal
mode output from an Nd:YLF Q-switched oscillator has been demonstrated by
injection locking to a low-power single-frequency master oscillator, this technique
requires careful mode matching between the master and slave oscillators and active
cavity length stabilization of the Q-switched slave oscillator [35]. A simpler method
of achieving single-frequency output was chosen for this application by using a
variation of the electronic linewidth narrowing technique [36, 37]. In this method,
very low power oscillation is allowed to build up in the Q-switched cavity over an
extended period of time (1–2 μs). By placing a frequency-selective element such as
an etalon in the cavity, this long buildup time and the corresponding many passes
through the etalon results in single longitudinal mode oscillation. The intracavity
power is monitored by the leakage through the high reflectivity (HR) mirror; when it
peaks in a weak relaxation oscillation, the Q-switch is opened. The low-power
single-frequency flux then serves to seed the buildup of a high-power Q-switched
pulse.

The output of the single-frequency Nd:YLF Q-switched oscillator is amplified to
~ 100 mJ using additional Nd:YLF preamplification. The beam is then
anamorphically expanded to match the aspect ratio of the extracted aperture of
the zigzag slab. A slightly oversized elliptical beam is clipped by a hard rectangular
aperture and relayed to a point conjugate to an image plane in the slab as depicted in
Fig. 5.5. In order to efficiently extract the stored energy in the slab amplifier in eight
gain passes, an injected seed energy of ~ 60 mJ is required.

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