Phase Conjugate Laser Optics

Chapter 5 - High-Pulse-Energy Phase Conjugated Laser System

C. BRENT DANE and LLOYD A. HACKEL
Lawrence Livermore National Laboratory, Livermore, California 94550, USA


5.1   INTRODUCTION

There are a number of important applications that require both high pulse energy
(>25 J/pulse) and high average power (>100 W) from a solid-state laser system.
Among examples of these are the generation of X rays for photolithography [1] and
the coherent illumination of distant objects for high-resolution imaging [2]. An
important and growing application of these lasers is the strengthening of metal parts
against stress corrosion cracking and fatigue failure by laser shock processing, often
referred to as laser peening [3]. High pulse energies are also useful for Raman
frequency conversion [4] and SBS pulse compression [5]. Another effective use is
the high-throughput optical conditioning and damage testing of large optics required
for large fusion driver lasers [6]. Outside of the devices with up to 100 J/pulse
presented in this chapter, high-pulse-energy solid-state laser systems have very low
pulse repetition frequencies (<0.1 Hz) or can only be operated in a single-shot
mode. For example, a diode-pumped 100-Hz, 1-kW system has been demonstrated,
but even in this case the pulse energies were limited to <10 J [7]. In this chapter we
will describe laser systems with pulse energies in the range of 25 to 100 J and
average powers spanning 100 to 1000 W. These systems use SBS phase conjugation
in master oscillator power amplifier (MOPA) geometries and have pulse durations
between 15 ns and 1 μs with near diffraction-limited divergence and transform-limited
bandwidth.

High-pulse-energy, high-average-power operation of a solid-state laser system is
a unique regime with very specific design requirements. The key enabling
technologies for the successful development of these systems are the face-pumped
zigzag slab amplifier architecture [8] and SBS phase conjugation. Accurate
wavefront correction is not just a requirement dictated by the divergence needs of an
intended application of the laser. High-beam-quality operation is first necessary for
high-average-power operation with high pulse energies, providing optimal amplifier
beam fill and optical extraction as well as preventing damage to optical components.
In addition to the low output divergence enabled by nonlinear phase conjugation,
other benefits include very high pulse-to-pulse and long-term beam pointing
stability as well as the ability to phase-lock multiple amplifier apertures to generate
even higher-energy beams. High beam quality also provides the option of very
efficient harmonic wavelength conversion.

Although the Nd:glass gain medium exhibits a lower fracture strength and lower
thermal conductivity than do crystalline materials such as Nd:YAG, its availability
in large volumes and its small cross section for stimulated emission
(3.5 × 10-20 cm2) make it well-suited to the storage requirements of high energy
per pulse operation. At the same time, the high saturation fluence for Nd-doped
phosphate glass and the potentially large thermally induced distortions resulting
from its low thermal conductivity offer a significant challenge for the operation of a
high-average-power amplifier system. Good thermal management in the form of
uniform pumping deposition, uniform cooling, and an optimized amplifier slab
design is crucial to successful high-power operation. Even under ideal conditions,
the high fluence required for efficient energy extraction requires carefully designed
beam transport and the accurate correction of the remaining thermally induced
wavefront aberrations in the amplifier medium in order to avoid damage to optical
components. For this reason, the flashlamp-pumped Nd:glass amplifier system has
been a valuable test bed for the development of high-average-power solid-state
amplifier architectures. The result has been robust optical designs that are also
readily applicable to high-average-power diode-pumped crystalline amplifier
systems having lower optical fluences. We believe that through this development
work, a number of valuable design principles have resulted which are directly
applicable to SBS phase conjugated MOPA architectures in general, and these will
be reviewed at the end of the chapter.

To illustrate the design principles for a high-pulse-energy, high-average-power,
SBS phase conjugated MOPA, we have chosen to present summarized technical
descriptions of three laser systems. Each of these shares a common flashlamp-
pumped Nd:glass amplifier design operating at 1053 nm [9]. The first system is a 25-
J/pulse, 15-ns laser using a liquid SBS phase conjugate mirror. The second extends
this pulse duration to 500 ns and uses a high-pressure-gas SBS cell with a self-
pumped four-wave-mixing loop geometry to lower the phase conjugation threshold
and to provide narrow spectral bandwidth. Finally, the third system coherently
combines four amplifier apertures using SBS phase-locking to increase the pulse
energy to 100 J/pulse. Each builds on the technology of the previous system, and
emphasis will be placed on the novel developments required for the laser under
discussion.

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