Phase Conjugate Laser Optics

Chapter 7 - Stimulated Brillouin Scattering Pulse Compression and Its Application in Lasers

G. A. PASMANIK, E. I. SHKLOVSKY, and A. A. SHILOV
Passat, Toronto, Ontario, Canada M3J 3H9

7.1   INTRODUCTION

Temporal laser pulse compression through stimulated scattering has a long history,
and its first observations [1–3] predate pioneering experiments on optical phase
conjugation [4]. Despite early history of optical pulse compression, study of
Brillouin compression began in earnest only after the well-known work of D. T. Hon
[5]. It was as a part of this work that the SBS method was first applied to an Nd:YAG
laser with the stated aim of shortening the pulse width in a double-pass power
amplifier with phase conjugate (PC) Brillouin mirror. This classical work had the
effect of inspiring further research of optical schemes for pulse compression as well
as its applications ranging from generation of new wavelengths through nonlinear
optical processes to laser-plasma-driven soft X-ray sources. Even though the main
characteristics of SBS pulse compression were established some 20 years ago
[6–20], SBS pulse compression-related research and literature remained intensely
active until the early 1990s, after which a noticeable drop in the level of SBS pulse
compression-related research was seen. To some degree, this decline in activity was
a natural outcome of the work of the early 1990s in which the physics of optical
pulse compression was well-defined. As well, the decline could be partially
attributed to the nearly routine application of the phenomenon in laser systems and
applications that followed. But beyond these factors, the rapid development of
diode-pump technology has also played a role, resulting in the appearance of
miniature solid-state lasers such as microchip lasers, capable of generating pulses
with durations of 1 ns and less [21–23]. For powerful diode-pumped and excimer
laser systems, however, SBS pulse compression still provides a viable, effective
option for short laser pulse generation.

It was shown almost two decades ago that a nanosecond laser pulse can be
compressed to a few hundreds of picoseconds [24]. Given that the typical pulse
width of diode-pumped Nd:YAG lasers is some nanoseconds in duration, Brillouin
scattering provides a very attractive way of compressing a backward Stokes pulse to
the subphonon lifetime region [25]. This approach still awaits common applications
in such systems.

During the years following the first work in Brillouin pulse compression, various
passive pulse compression schemes have been studied, including truncated SBS
[26–31], two-step Brillouin compression [32, 33] and combined SBS–SRS
compression—the latter comprising cascaded Brillouin and Raman compressors
[34–39].

In the following sections we describe key experimental and theoretical studies as
well as results from numerical simulations of laser pulse compression accompanying
backward SBS. Since in many cases the choice of SBS-active material is crucial for
efficient pulse compression, we outline selection criteria and discuss competing
physical–optical processes that should be taken into account when selecting the
pulse compressor medium. We also describe experimental results of cascaded SBS–
SRS compression as well as application of this technique to the generation of
picosecond pulses.

While we have endeavored to provide a well-rounded discussion of this field, the
space restrictions inevitably limit the length of the discussion in this chapter. The
authors regret that much of the worthy work that has been advanced in this field
cannot be included here, but they also feel that the sheer size of the literature argues
for the abiding interest in this area of physical optics.

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