In this chapter we introduce the concept of Brillouin optomechanics, a phonon-photon interaction process mediated by the electrostrictive force exerted by light on dielectrics and the photoelastic scattering of light from an acoustic wave. We first provide a review of the phenomenon and continue with the first experiments where stimulated Brillouin optomechanical actuation was used in microdevices, and spontaneous Brillouin cooling was demonstrated.
IntroductionStimulated Brillouin scattering (SBS) [1,2] has been used since the 1960s as an acousto-optic gain mechanism for lasers [3]. Subsequently, it has been employed as a tool for slow light [4], for non-destructive characterization of materials [5][6][7], and in optical phase conjugation [8] for holography. Brillouin lasers, due to their narrow linewidth, are also employed in ring laser gyroscopes [9]. On the other hand, in fiber-based communication systems and high power fiber lasers, SBS is considered an undesirable mechanism that interferes with proper function [10]. It is important to note that SBS is an optical nonlinearity common to all dielectrics in all states of matter, and is generally considered to be the strongest optical nonlinearity [11]. In addition to optical fibers and bulk media SBS has been demonstrated in a variety of optical systems. Examples range over a variety of size scales, including nanoscale spheres [12], fluid droplets [13], photonic-crystal fibers [14], and recently in mm-scale [15,16] and micron-scale resonators [17].