Phase Conjugate Laser Optics

Chapter 3 - Laser Resonators with Brillouin Mirrors

MARTIN OSTERMEYER and RALF MENZEL
University of Potsdam, Institute of Physics, Chair of Photonics, 14469 Potsdam, Germany


3.1  INTRODUCTION

As has been shown in the preceding chapter, nonlinear mirrors based on stimulated
Brillouin scattering (SBS mirrors) can be used to produce the phase conjugate of a
wavefront [1, 2] with a fidelity close to one. There are two major different ways of
realizing high-power lasers with excellent beam quality (high-brightness lasers).
One is the laser oscillator, and the second is the master oscillator power amplifier
concept (MOPA). Depending on the specific application, either the laser oscillator or
the MOPA concept might be more appropriate. Phase conjugating SBS mirrors can
be applied in both designs to compensate for phase distortions in the laser-active
medium. Especially in solid-state lasers where the thermal load due to the pump is a
serious problem, these concepts to improve the beam quality can be useful. The
phase conjugating SBS mirror is easy to use since it is self-pumped by the incident
beam. However, if SBS-phase conjugation is applied inside a laser resonator, a
more elaborate Brillouin-enhanced four-wave mixing (BEFWM) scheme is the
appropriate description of the physical process. As a consequence, the threshold of
bulk SBS mirrors is decreased if they are placed in a resonator.

The motivation to use a phase conjugating mirror (PCM) within a laser resonator
or simply to replace one of the resonator mirrors by the PCM is at least twofold.
Besides the compensation of phase distortions to achieve an excellent beam quality,
also the stability of phase conjugate resonators (PCR) is guaranteed and independent
from the specific resonator design (see Section 3.3). Thus, fluctuating or drifting
optical parameters in the laser resonator such as a fluctuating thermal lens in a solid-
state laser can be dynamically corrected in a properly designed PCR. As a result, the
beam parameters of the solid-state laser will be independent of the pump power. A
further consequence is that the misalignment sensitivity of the resonator is reduced.

If the PCM is based on SBS apart from these two complexes known as aberration
compensation and resonator stability, there are other motives arising to use such an
SBS mirror in addition. For instance, the frequency shifting effect of the SBS mirror
can be used to generate a large bandwidth and short pulses in injected resonators
[3, 4] (see Section 3.6.1) or it can be used to avoid gain competition for counter-
propagating waves in the laser-active material [5, 6] (see Section 3.2). The nonlinear
properties of the SBS mirror inside the resonator (see previous chapter) give the
opportunity for two major applications. One is Q-switching the laser resonator (see
Section 3.4). Secondly, amplified spontaneous emission (ASE) can be avoided, for
example, in regenerative amplifiers [7–13], but regenerative amplifiers are not dealt
with here. To decrease the threshold of bulk SBS mirrors, they were placed in
resonators just by themselves. Again for these techniques the reader is referred to the
original literature [14–18].

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