The integration of optomechanically coupled photonic crystal cavities to indium arsenide quantum dots is studied experimentally and theoretically. Electrostatic tuning results for one-and twodimensional photonic crystals are presented. c ⃝ 2010 Optical Society of America OCIS codes: (120.4880) Optomechanics; (230.5590) Quantum-well, -wire and -dot devices A significant challenge in the development of coherent device physics using self-assembled semiconductor quantum dots (QDs) is the wide distribution of transition energies from dot-to-dot on a given sample. This inhomogeneity stems from random nucleation during the island formation stage of growth [1]. Thus, a tunable architecture is necessary when resonantly addressing single QDs with a photonic device. Techniques such as temperature [2,3], digital etch [4], stark shift [5], and thin-film vapor condensation [6,7] tuning have been successfully utilized to scan the detuning of nanocavities to single QDs in cavity quantum electrodynamics (QED) experiments, but have the drawbacks of being slow and limited in tuning range, and can contribute to deterioration of the QD and cavity. Recent progress in optomechanical systems suggests exceptional methods of accessing the strongly-coupled exciton-photon regime. In particular, the extremely large optomechanical couplings (g) and optical quality factors (Q) observed in one-dimensional "zipper" [8,9] and two-dimensional slotted [10] photonic crystals, when integrated with microelectromechanical systems (MEMS), can provide fast, wide-range, in-situ, continuous wavelength tuning to QD emission lines.A scanning electron microscope (SEM) micrograph of an InP-quantum-well-based tunable zipper cavity is shown in Fig. 1(a). The device is comprised of a pair of doubly-clamped photonic crystal nanobeams, with a lattice variation in the center of the beams to confine the optical modes [8] . These localized resonances are coupled to the inter-beam gap x g through the optomechanical coupling g = dω/dx, where ω is the frequency of the cavity mode and x is the relative displacement of the beams from the original gap x g . Metal electrodes are deposited on the ends of the beams, enabling tuning of x g , and therefore the resonant optical wavelength [9]. As seen in the micro-photoluminescence (PL) spectra in Fig. 1(c)