The field of optomechanics provides us with several examples of quantum photon-phonon interface. In this paper, we theoretically investigate the generation and manipulation of quantum correlations in a microfabricated optomechanical array. We consider a system consisting of localized photonic and phononic modes interacting locally via radiation pressure at each lattice site with the possibility of hopping of photons and phonons between neighboring sites. We show that such an interaction can correlate various modes of a driven coupled optomechanical array with well-chosen system parameters. Moreover, in the linearized regime of Gaussian fluctuations, the quantum correlations not only survive in the presence of thermal noise, but may also be generated thermally. We find that these optomechanical arrays provide a suitable platform for quantum simulation of various many-body systems.
I. INTRODUCTIONThe impressive experimental progress in fabricating micromechanical and nanomechanical devices have opened a route towards the exhibition of quantum behavior at macroscopic scales. The interaction between micro-or nanomechanical oscillators and the optical field via the radiation pressure force is the basis of a wide variety of optomechanical phenomena. Despite their variety in the system sizes, parameters, and configurations, optomechanical systems (OMSs) share common features. Almost all OMSs are described by the same physics. OMSs offer further insights into the issues concerning the development of quantum memory for quantum computers [1], high precision position, mass or force sensing [2-6], quantum transducers [7], classical and quantum communication [8], ground state cooling of mechanical oscillators [9,10], nonclassical correlations between single photons and phonons [11], generation of nonclassical states [12] and testing of the foundations of quantum mechanics [13][14][15][16]. For a recent review and current areas of focus of quantum optomechanics see Refs. [17,18].The extension to multimode systems is an attractive route for quantum optomechanics. A group of mechanical oscillators interacting via the radiation pressure with a common optical mode [19][20][21][22][23][24][25][26], or a group of mechanical oscillators locally interacting with a single optical mode involving the tunneling of photons and phonons between neighboring sites [27][28][29][30][31][32][33][34][35][36][37][38] are the two realizations of multimode optomechanics. The former is realized in a single optical cavity containing multiple membranes while the latter is realized experimentally in the so-called optomechanical crystals (OMCs) in one and two *