Phase Conjugate Laser Optics

Chapter 5.4 - A Long Pulse 500-NS, 30-J Laser System

5.4   A LONG PULSE 500-NS, 30-J LASER SYSTEM

5.4.1   Design considerations for the 500-ns system

In laser illumination applications such as long-range coherent radar or high-
resolution speckle imaging [2], a narrow-bandwidth, high-pulse-energy output is
needed, often with pulse widths in the range of 500 ns to 1 μs. These applications
require the near-constant output power provided by a quasi-rectangular temporal
pulse shape. The optimization of nonlinear frequency conversion processes such as
harmonic generation or the pumping of an optical parametric oscillator (OPO) also
benefits from this pulse shape. In addition to its use as a laser illuminator, the
efficient operation of a high-pulse-energy, high-average-power, long-pulse laser
system provides the potential for other applications for which the lower peak power
improves radiation coupling and raises the optical damage threshold of materials.
Examples include medical applications, the annealing of amorphous semiconductor
coatings, and pumping other laser amplifiers such as Ti:sapphire or liquid dye.

The goal of >500-ns pulse duration is significantly longer than the 5–30 ns
generally available from the Q-switched operation of solid-state lasers, although
some work has been reported on the generation of long pulses. Long-pulse
oscillators emitting near-rectangular pulses have been demonstrated by
suppressing the relaxation oscillation behavior (temporal spiking) typical of
solid-state lasers. This has been accomplished by actively varying the intracavity
loss during the laser pulse either with closed-loop feedback on the output power
[42] or with a preprogrammed temporal shape [43]. In both cases, pulse widths of
up to 600 ns were achieved. However, the sensitivity and temporal bandwidth
required for these control schemes are often difficult to achieve even in a
carefully controlled laboratory environment. Long pulses have also been
generated with passive control using an intracavity saturable absorber. In this
manner, pulse widths of up to 500 ns were demonstrated but with a peaked
temporal profile, large shot-to-shot pulse width variations (100-ns RMS), and a
pulse energy of only 0.2 mJ [44].

The pulse energy requirements of a long-range illuminator (>10 J) make a
master-oscillator power amplifier (MOPA) the most practical laser architecture. The
design goal for the laser amplifier output that is presented here was 30 J / pulse at
1 μm. The large amount of amplification required to reach this energy from a low-
energy injected oscillator pulse leads to severe temporal distortion of the input pulse
shape due to amplifier gain saturation during efficient optical extraction. For this
reason, the near-rectangular output of previously reported that long-pulse oscillators
would not be suitable as an injection source. It has been recognized, however, that
the smooth temporal profile of a relaxation oscillation pulse emitted by a free-
running solid-state laser suffers much less pulse-width distortion when amplified
[45]. Applying this concept, 1.1 J in a 110-ns pulse was demonstrated from a single
amplifier aperture that was then frequency-doubled to 520 mJ at 532 nm [46]. The
temporal profile remained, however, near Gaussian in shape.

For this laser system, we adopted a scheme that also relies on the amplification
of the output of a free-running master oscillator [32]. However, only the leading
edge of the pulse is used and it will be shown that the measured width of the injected
pulse does not directly determine the width of the amplified output pulse. The
amplification of the leading edge of the input pulse gives rise to a quasi-constant
output power, the magnitude of which is dependent on the exponential time constant
of this rising edge. A simple analytical theory allows the power, and hence pulse
duration, to be tailored to a desired level by adjusting the optical buildup time in the
oscillator.

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